Optical image capturing module

ABSTRACT

An optical image capturing module includes a lens assembly and a circuit assembly including a circuit substrate having multiple circuit contacts, an image sensing component having multiple image contacts, and a sensor holder. The image contacts are electrically connected to the circuit contacts via signal transmission elements embedded in the sensor holder. The sensor holder covers the circuit contacts and the image contacts. The lens assembly includes a lens base disposed on the circuit substrate and a lens group. The lens base has a receiving hole penetrating through two ends thereof, thereby the lens base is hollow. The image sensing component is located in the receiving hole. The lens group including at least two lenses having refractive power is disposed on the lens base and is located in the receiving hole, thereby light could pass through the lens group and project onto a sensing surface of the image sensing component.

BACKGROUND OF THE INVENTION Technical Field

The present invention generally relates to an optical image capturingmodule, and more particularly to a compact optical image capturingmodule for an electronic device.

Description of Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of the ordinaryphotographing camera is commonly selected from charge coupled device(CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor).Also, as advanced semiconductor manufacturing technology enables theminimization of the pixel size of the image sensing device, thedevelopment of the optical image capturing system towards the field ofhigh pixels. Therefore, the requirement for high imaging quality israpidly raised.

The conventional optical system of the portable electronic deviceusually has five or sixth lenses. However, the optical system is askedto take pictures in a dark environment, in other words, the opticalsystem is asked to have a large aperture. The conventional opticalsystem provides high optical performance as required.

It is an important issue to increase the quantity of light entering thelens. Also, the modern lens is also asked to have several characters,including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing module which use structural size design and combinationof refractive powers, convex and concave surfaces of at least twooptical lenses (the convex or concave surface in the disclosure denotesthe geometrical shape of an image-side surface or an object-side surfaceof each lens on an optical axis) to reduce the size and increase thequantity of incoming light of the optical image capturing module,thereby the optical image capturing module could has a better amount oflight entering therein and could improve imaging total pixels andimaging quality for image formation, so as to be applied to minimizedelectronic products.

The term and its definition to the structural component parameter in theembodiment of the present are shown as below for further reference.

Take FIG. 1A as an example to illustrate the structural component of theoptical image capturing module. The optical image capturing modulemainly includes a circuit assembly and a lens assembly, wherein thecircuit assembly includes a circuit substrate EB, an image sensingcomponent S, and a sensor holder SB. In the present invention, the imagesensing component S is fixed on the circuit substrate in a Chip On Board(COB) package.

The lens assembly includes a lens base LB1 and a lens group L, whereinthe lens base LB1 is made of metal (such as aluminum, copper, silver,gold, and etc.), plastic (e.g. polycarbonate (PC)), or liquid crystalplastic (LCP), which are opaque materials. In addition, a maximum valueof a minimum length on a periphery of the lens base LB1 perpendicular toan optical axis of the lens group L is denoted by PhiD, wherein the lensbase LB1 has a receiving hole penetrating through both ends thereof tobe hollow. The lens base LB1 is disposed on the sensor holder SB, sothat the receiving hole directly faces the image sensing component S.More specifically, the lens base LB1 has a lens holder LH1 and a lensbarrel B1, wherein the lens holder LH1 is hollow and is opaque, and thelens barrel B1 is hollow and is opaque and is disposed in the lensholder LH1. An inside of the lens barrel B1 and the lens holder LH1constitute the receiving hole. Moreover, a maximum thickness of the lensholder LH1 is denoted by TH1, and a minimum thickness of the lens barrelB1 is denoted by TH2.

The lens group L includes at least two lenses with refractive powerwhich are disposed on the lens base LB1 and are located in the receivinghole. The term and its definition to the lens parameter in theembodiment of the present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

A maximum height for image formation of the optical image capturingmodule is denoted by HOI. A height of the optical image capturing module(i.e., a distance between an object-side surface of the first lens andan image plane on an optical axis) is denoted by HOS. A distance fromthe object-side surface of the first lens to the image-side surface ofthe seventh lens is denoted by InTL. A distance from the first lens tothe second lens is denoted by IN12 (instance). A central thickness ofthe first lens of the optical image capturing module on the optical axisis denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing moduleis denoted by NA1 (instance). A refractive index of the first lens isdenoted by Nd1 (instance).

The lens parameter related to a view angle of the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing module isdenoted by HEP. For any surface of any lens, a maximum effective halfdiameter (EHD) is a perpendicular distance between an optical axis and acrossing point on the surface where the incident light with a maximumviewing angle of the optical image capturing module passing the veryedge of the entrance pupil. For example, the maximum effective halfdiameter of the object-side surface of the first lens is denoted byEHD11, the maximum effective half diameter of the image-side surface ofthe first lens is denoted by EHD12, the maximum effective half diameterof the object-side surface of the second lens is denoted by EHD21, themaximum effective half diameter of the image-side surface of the secondlens is denoted by EHD22, and so on. In the optical image capturingmodule, a maximum effective diameter of the image-side surface of thelens closest to the image plane is denoted by PhiA, which satisfies thecondition: PhiA=2*EHD. If the surface is aspherical, a cut-off point ofthe largest effective diameter is the cut-off point containing theaspheric surface. An ineffective half diameter (IHD) of any surface ofone single lens refers to a surface segment between cut-off points ofthe maximum effective half diameter of the same surface extending in adirection away from the optical axis, wherein said a cut-off point is anend point of the surface having an aspheric coefficient if said surfaceis aspheric. In the optical image capturing module, a maximum diameterof the image-side surface of the lens closest to the image plane isdenoted by PhiB, which satisfies the condition: PhiB=2*(maximumeffective half diameter EHD+maximum ineffective half diameterIHD)=PhiA+2*(maximum ineffective half diameter IHD).

In the optical image capturing module, a maximum effective diameter ofthe image-side surface of the lens closest to the image plane (i.e., theimage space) could be also called optical exit pupil, and is denoted byPhiA. If the optical exit pupil is located on the image-side surface ofthe third lens, then it is denoted by PhiA3; if the optical exit pupilis located on the image-side surface of the fourth lens, then it isdenoted by PhiA4; if the optical exit pupil is located on the image-sidesurface of the fifth lens, then it is denoted by PhiA5; if the opticalexit pupil is located on the image-side surface of the sixth lens, thenit is denoted by PhiA6, and so on. A pupil magnification ratio of theoptical image capturing module is denoted by PMR, which satisfies thecondition: PMR=PhiA/HEP.

The lens parameter related to an arc length of the shape of a surfaceand a surface profile:

For any surface of any lens, a profile curve length of the maximumeffective half diameter is, by definition, measured from a start pointwhere the optical axis of the belonging optical image capturing modulepasses through the surface of the lens, along a surface profile of thelens, and finally to an end point of the maximum effective half diameterthereof. In other words, the curve length between the aforementionedstart and end points is the profile curve length of the maximumeffective half diameter, which is denoted by ARS. For example, theprofile curve length of the maximum effective half diameter of theobject-side surface of the first lens is denoted by ARS11, the profilecurve length of the maximum effective half diameter of the image-sidesurface of the first lens is denoted by ARS12, the profile curve lengthof the maximum effective half diameter of the object-side surface of thesecond lens is denoted by ARS21, the profile curve length of the maximumeffective half diameter of the image-side surface of the second lens isdenoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of theentrance pupil diameter (HEP) is, by definition, measured from a startpoint where the optical axis of the belonging optical image capturingmodule passes through the surface of the lens, along a surface profileof the lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis. In other words, the curve length between theaforementioned stat point and the coordinate point is the profile curvelength of a half of the entrance pupil diameter (HEP), and is denoted byARE. For example, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the first lens isdenoted by ARE11, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the first lens isdenoted by ARE12, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the second lens isdenoted by ARE21, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the second lens isdenoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the sixthlens, which is passed through by the optical axis, to a point on theoptical axis, where a projection of the maximum effective semi diameterof the object-side surface of the sixth lens ends, is denoted by InRS61(the depth of the maximum effective semi diameter). A displacement froma point on the image-side surface of the sixth lens, which is passedthrough by the optical axis, to a point on the optical axis, where aprojection of the maximum effective semi diameter of the image-sidesurface of the seventh lens ends, is denoted by InRS62 (the depth of themaximum effective semi diameter). The depth of the maximum effectivesemi diameter (sinkage) on the object-side surface or the image-sidesurface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens,and the tangent point is tangent to a plane perpendicular to the opticalaxis and the tangent point cannot be a crossover point on the opticalaxis. Following the above description, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens and the optical axis is HVT51 (instance), and a distanceperpendicular to the optical axis between a critical point C52 on theimage-side surface of the fifth lens and the optical axis is HVT52(instance). A distance perpendicular to the optical axis between acritical point C61 on the object-side surface of the sixth lens and theoptical axis is HVT61 (instance), and a distance perpendicular to theoptical axis between a critical point C62 on the image-side surface ofthe sixth lens and the optical axis is HVT62 (instance). A distanceperpendicular to the optical axis between a critical point on theobject-side or image-side surface of other lenses is denoted in the samemanner.

The object-side surface of the seventh lens has one inflection pointIF711 which is nearest to the optical axis, and the sinkage value of theinflection point IF711 is denoted by SGI711 (instance). A distanceperpendicular to the optical axis between the inflection point IF711 andthe optical axis is HIF711 (instance). The image-side surface of theseventh lens has one inflection point IF721 which is nearest to theoptical axis, and the sinkage value of the inflection point IF721 isdenoted by SGI721 (instance). A distance perpendicular to the opticalaxis between the inflection point IF721 and the optical axis is HIF721(instance).

The object-side surface of the seventh lens has one inflection pointIF712 which is the second nearest to the optical axis, and the sinkagevalue of the inflection point IF712 is denoted by SGI712 (instance). Adistance perpendicular to the optical axis between the inflection pointIF712 and the optical axis is HIF712 (instance). The image-side surfaceof the seventh lens has one inflection point IF722 which is the secondnearest to the optical axis, and the sinkage value of the inflectionpoint IF722 is denoted by SGI722 (instance). A distance perpendicular tothe optical axis between the inflection point IF722 and the optical axisis HIF722 (instance).

The object-side surface of the seventh lens has one inflection pointIF713 which is the third nearest to the optical axis, and the sinkagevalue of the inflection point IF713 is denoted by SGI713 (instance). Adistance perpendicular to the optical axis between the inflection pointIF713 and the optical axis is HIF713 (instance). The image-side surfaceof the seventh lens has one inflection point IF723 which is the thirdnearest to the optical axis, and the sinkage value of the inflectionpoint IF723 is denoted by SGI723 (instance). A distance perpendicular tothe optical axis between the inflection point IF723 and the optical axisis HIF723 (instance).

The object-side surface of the seventh lens has one inflection pointIF714 which is the fourth nearest to the optical axis, and the sinkagevalue of the inflection point IF714 is denoted by SGI714 (instance). Adistance perpendicular to the optical axis between the inflection pointIF714 and the optical axis is HIF714 (instance). The image-side surfaceof the seventh lens has one inflection point IF724 which is the fourthnearest to the optical axis, and the sinkage value of the inflectionpoint IF724 is denoted by SGI724 (instance). A distance perpendicular tothe optical axis between the inflection point IF724 and the optical axisis HIF724 (instance).

An inflection point, a distance perpendicular to the optical axisbetween the inflection point and the optical axis, and a sinkage valuethereof on the object-side surface or image-side surface of other lensesis denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturingmodule is denoted by ODT. TV distortion for image formation in theoptical image capturing module is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100% field. An offset of the spherical aberration is denoted by DFS.An offset of the coma aberration is denoted by DFC.

The present invention provides an optical image capturing module, whichis capable of focusing visible and infrared (i.e., dual-mode) at thesame time and achieving certain performance, wherein the sixth lensthereof is provided with an inflection point at the object-side surfaceor at the image-side surface to adjust the incident angle of each viewfield and modify the ODT and the TDT. In addition, the surfaces of thesixth lens are capable of modifying the optical path to improve theimagining quality.

The optical image capturing module of the present invention includes acircuit assembly and a lens assembly. The circuit assembly includes acircuit substrate, a sensor holder, and an image sensing component,wherein the circuit substrate has a plurality of circuit contactsthereon. The image sensing component has a first surface and a secondsurface, wherein the first surface is connected to the circuitsubstrate. The second surface has a sensing surface and a plurality ofimage contacts. Each of the image contacts is electrically connected toone of the circuit contacts on the circuit substrate via a plurality ofsignal transmission elements. The sensor holder is disposed on thecircuit substrate and on the second surface of the image sensingcomponent, and covers the circuit contacts and the image contacts. Thesignal transmission elements are embedded in the sensor holder. The lensassembly includes a lens base and a lens group, wherein the lens base ismade of an opaque material and has a receiving hole penetrating throughtwo ends of the lens base, so that the lens base is hollow. The lensbase is disposed on the sensor holder, so that the receiving holedirectly faces the image sensing component. The lens group includes atleast two lenses having refractive power, and is disposed on the lensbase and is located in the receiving hole. An image plane of the lensgroup is located on the sensing surface, and an optical axis of the lensgroup overlaps with a central normal of the sensing surface, so that alight passes through the lens group in the receiving hole and projectsonto the sensing surface. The optical image capturing module furthersatisfies:

1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; 0 mm<PhiD≤18 mm; 0<PhiA/PhiD≤0.99;and 0.9≤2(ARE/HEP)≤2.0;

where f is a focal length of the lens group; HEP is an entrance pupildiameter of the lens group; HAF is a half of a maximum field angle ofthe lens group; PhiD is a maximum value of a minimum length on aperiphery of the lens base perpendicular to the optical axis of the lensgroup; PhiA is a maximum effective diameter of an image-side surface ofthe at least two lenses of the lens group closest to the image plane;ARE is a profile curve length measured from a start point where theoptical axis of the lens group passes through any surface of one of theat least two lenses, along a surface profile of the corresponding lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis.

The length of the contour curve of any surface of a single lens in therange of the maximum effective radius affects the surface correctionaberration and the optical path difference between the fields of view.The longer the profile curve length, the better the ability to correctthe aberration, but at the same time It will increase the difficulty inmanufacturing, so it is necessary to control the length of the profilecurve of any surface of a single lens within the maximum effectiveradius, in particular to control the profile length (ARS) and thesurface within the maximum effective radius of the surface. Theproportional relationship (ARS/TP) between the thicknesses (TP) of thelens on the optical axis. For example, the length of the contour curveof the maximum effective radius of the side surface of the first lensobject is represented by ARS11, and the thickness of the first lens onthe optical axis is TP1, and the ratio between the two is ARS11/TP1, andthe maximum effective radius of the side of the first lens image side.The length of the contour curve is represented by ARS12, and the ratiobetween it and TP1 is ARS12/TP1. The length of the contour curve of themaximum effective radius of the side of the second lens object isrepresented by ARS21, the thickness of the second lens on the opticalaxis is TP2, the ratio between the two is ARS21/TP2, and the contour ofthe maximum effective radius of the side of the second lens image Thelength of the curve is represented by ARS22, and the ratio between itand TP2 is ARS22/TP2. The proportional relationship between the lengthof the profile of the maximum effective radius of any surface of theremaining lenses in the optical imaging system and the thickness (TP) ofthe lens on the optical axis to which the surface belongs, and so on.The optical image capturing module of the present invention satisfies:0.9≤ARS/EHD≤2.0.

The optical image capturing module has a maximum image height HOI on theimage plane vertical to the optical axis. A transverse aberration at 0.7HOI in the positive direction of the tangential ray fan aberration afterthe longest operation wavelength passing through the edge of theentrance pupil is denoted by PLTA; a transverse aberration at 0.7 HOI inthe positive direction of the tangential ray fan aberration after theshortest operation wavelength passing through the edge of the entrancepupil is denoted by PSTA; a transverse aberration at 0.7 HOI in thenegative direction of the tangential ray fan aberration after thelongest operation wavelength passing through the edge of the entrancepupil is denoted by NLTA; a transverse aberration at 0.7 HOI in thenegative direction of the tangential ray fan aberration after theshortest operation wavelength passing through the edge of the entrancepupil is denoted by NSTA; a transverse aberration at 0.7 HOI of thesagittal ray fan aberration after the longest operation wavelengthpassing through the edge of the entrance pupil is denoted by SLTA; atransverse aberration at 0.7 HOI of the sagittal ray fan aberrationafter the shortest operation wavelength passing through the edge of theentrance pupil is denoted by SSTA. The optical image capturing module ofthe present invention satisfies:

PLTA≤100 μm; PSTA≤100 μm; NLTA≤100 μm; NSTA≤100 μm; SLTA≤100 μm;SSTA≤100 μm; |TDT|<250%; 0.1≤InTL/HOS≤0.95; and 0.2≤Ins/HOS≤1.1.

For visible light spectrum, the values of MTF in the spatial frequencyof 110 cycles/mm at the optical axis, 0.3 field of view, and 0.7 fieldof view on an image plane are respectively denoted by MTFQ0, MTFQ3, andMTFQ7. The optical image capturing module of the present inventionsatisfies:

MTFQ0≥0.2; MTFQ3≥0.01; and MTFQ7≥0.01.

For any surface of any lens, the profile curve length within a half ofthe entrance pupil diameter (HEP) affects the ability of the surface tocorrect aberration and differences between optical paths of light indifferent fields of view. With longer profile curve length, the abilityto correct aberration is better. However, the difficulty ofmanufacturing increases as well. Therefore, the profile curve lengthwithin a half of the entrance pupil diameter (HEP) of any surface of anylens has to be controlled. The ratio between the profile curve length(ARE) within a half of the entrance pupil diameter (HEP) of one surfaceand the thickness (TP) of the lens, which the surface belonged to, onthe optical axis (i.e., ARE/TP) has to be particularly controlled. Forexample, the profile curve length of a half of the entrance pupildiameter (HEP) of the object-side surface of the first lens is denotedby ARE11, the thickness of the first lens on the optical axis is TP1,and the ratio between these two parameters is ARE11/TP1; the profilecurve length of a half of the entrance pupil diameter (HEP) of theimage-side surface of the first lens is denoted by ARE12, and the ratiobetween ARE12 and TP1 is ARE12/TP1. The profile curve length of a halfof the entrance pupil diameter (HEP) of the object-side surface of thesecond lens is denoted by ARE21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARE21/TP2; the profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the second lens is denotedby ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For anysurface of other lenses in the optical image capturing system, the ratiobetween the profile curve length of a half of the entrance pupildiameter (HEP) thereof and the thickness of the lens which the surfacebelonged to is denoted in the same manner.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to thefollowing detailed description of some illustrative embodiments inconjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first structural embodiment of thepresent invention;

FIG. 1B is a schematic diagram of a second structural embodiment of thepresent invention;

FIG. 1C is a schematic diagram of a third structural embodiment of thepresent invention;

FIG. 1D is a schematic diagram of a fourth structural embodiment of thepresent invention;

FIG. 1E is a schematic diagram of a fifth structural embodiment of thepresent invention;

FIG. 1F is a schematic diagram of a sixth structural embodiment of thepresent invention;

FIG. 1G is a schematic diagram of a seventh structural embodiment of thepresent invention;

FIG. 2A is a schematic diagram of a first optical embodiment of thepresent invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the first optical embodimentof the present application;

FIG. 3A is a schematic diagram of a second optical embodiment of thepresent invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the second optical embodimentof the present application;

FIG. 4A is a schematic diagram of a third optical embodiment of thepresent invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the third optical embodimentof the present application;

FIG. 5A is a schematic diagram of a fourth optical embodiment of thepresent invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the fourth optical embodimentof the present application;

FIG. 6A is a schematic diagram of a fifth optical embodiment of thepresent invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the fifth optical embodimentof the present application;

FIG. 7A is a schematic diagram of a sixth optical embodiment of thepresent invention;

FIG. 7B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingmodule in the order from left to right of the sixth optical embodimentof the present application;

FIG. 8A is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the mobile communicationdevice;

FIG. 8B is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the mobile informationdevice;

FIG. 8C is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the smart watch;

FIG. 8D is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the smart head-wearingdevice;

FIG. 8E is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the safety monitoringdevice;

FIG. 8F is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the vehicle image device;

FIG. 8G is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the unmanned aircraftdevice;

FIG. 8H is a schematic diagram, showing the optical image capturingmodule of the present invention is applied to the extreme sport imagedevice.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing module of the present invention includes astructural design and an optical design, wherein structural embodimentswill be described first.

As shown in FIG. 1A, an optical image capturing module according to afirst structural embodiment of the present invention includes mainlyincludes a circuit assembly and a lens assembly. The circuit assemblyincludes an image sensing component S, a sensor holder SB, and a circuitsubstrate EB. A maximum value of a minimum length of an outer peripheryof the image sensing component S which is perpendicular to a plane of anoptical axis of the lens assembly is denoted by LS. In the currentembodiment, the image sensing component S is fixed on the circuitsubstrate EB in a Chip On Board (COB) package. More specifically, thecircuit substrate EB has a plurality of circuit contacts EP thereon; theimage sensing component S has a first surface S1 and a second surfaceS2, wherein the first surface S1 is connected to the circuit substrateEB, and the second surface S2 has a sensing surface and a plurality ofimage contacts IP. Each of the image contacts IP is electricallyconnected to one of the circuit contacts EP on the circuit substrate EBvia a plurality of signal transmission elements SC1. The sensor holderSB is disposed on the circuit substrate EB and on the second surface S2of the image sensing component S, and covers the circuit contacts EP andthe image contacts IP. The signal transmission elements SC1 are embeddedin the sensor holder SB. In the current embodiment, each of the signaltransmission elements SC1 is a gold wire. In this way, when an imageoptical signal is sensed by the sensing surface of the image sensingcomponent S and is transformed into an electrical signal, the electricalsignal could be sent to the circuit contacts EP via the image contactsIP and the signal transmission elements SC1, so that the circuitcontacts EP could transmit the electrical signal to other externalcomponents for subsequent processing.

The lens assembly includes a lens base LB1, a lens group L, and anIR-cut filter IR1. In the current embodiment, the lens base LB1 is madeof plastic material and is opaque, and includes a lens holder LH1 and alens barrel B1. More specifically, the lens holder LH1 has apredetermined thickness TH1, and a maximum value of a minimum length ona periphery of the lens holder LH1 perpendicular to the optical axis ofthe lens group L is denoted by PhiD. In addition, the lens holder LH1has a lower through hole DH1 penetrating through both ends of the lensholder LH1 to be hollow, and is fixed on the sensor holder SB, so thatthe image sensing component S is located in the lower through hole DH1.The lens barrel B1 has a predetermined thickness TH2, and a maximumvalue of a minimum length on a periphery of the lens barrel B1perpendicular to the optical axis of the lens group L is denoted byPhiC. Moreover, the lens barrel B1 is disposed in the lens holder LH1 tobe located in the lower through hole DH1, and has an upper through holeUH1 penetrating through both ends of the lens barrel B1, so that theupper through hole UH1 communicates with the lower through hole DH1 toform a receiving hole, and the lens base LB1 is hollow, wherein theupper through hole UH1 of the lens barrel B1 directly faces the sensingsurface of the image sensing component S.

The lens group L includes at least two lenses with refractive power, andoptical embodiments will be described in detail later. The lens group Lis disposed on the lens barrel B1 of the lens base LB1 and is located inthe upper through hole UH1. In addition, an image plane of the lensgroup L is located on the sensing surface of the image sensing componentS, wherein the optical axis of the lens group L overlaps with a centralnormal of the sensing surface, so that light could pass through the lensgroup L in the receiving hole and could be projected onto the sensingsurface. Moreover, a maximum diameter of an image-side surface of a lensof the lens group L closest to the image plane is denoted by PhiB, and amaximum effective diameter of the image-side surface of the lens of thelens group L closest to the image plane (i.e., the image space) could bealso called optical exit pupil, and is denoted by PhiA.

The IR-cut filter IR1 is fixed on the lens holder LH1 of the lens baseLB1, and is located between the lens group L and the image sensingcomponent S, and is located above the image sensing component S, therebyto filter out an excess infrared in the image light passing through thelens group L, enhancing the image quality.

It is worth mentioning that, in order to overlap the optical axis of thelens group L with the central normal of the sensing surface of the imagesensing component S, an outer side of the lens barrel B1 of the opticalimage capturing module of the current embodiment is not completely incontact with an inner periphery of the lens holder LH1, thereby to leavea slight gap, so that a curable glue could be coated between the lensholder LH1 and the lens barrel B1 in advance, and the optical axis ofthe lens group L and the central normal of the image sensing component Scould be adjusted to be overlapped with each other, and then the curableglue is cured to fix the lens barrel B1 to the lens holder LH1, that is,an active alignment assembly is carried out. The precision optical imagecapturing modules or special applications (such as the assembly ofmultiple lenses) require the active alignment technology, and theoptical image capturing module of the present invention could meet suchrequirement.

In order to keep small in size and provide high imaging quality, theoptical image capturing module of the current embodiment satisfies:

0 mm<PhiA≤17.4 mm; 0 mm<PhiC≤17.7 mm; 0 mm<PhiD≤18 mm; 0 mm<TH1≤5 mm; 0mm<TH2≤5 mm; 0<PhiA/PhiD≤0.99; 0 mm<TH1+TH2≤1.5 mm; and0<2*(TH1+TH2)/PhiA≤0.95.

Preferably, the optical image capturing module of the current embodimentsatisfies:

0 mm<PhiA≤13.5 mm; 0 mm<PhiC≤14 mm; 0 mm<PhiD≤15 mm; 0 mm<TH1≤0.5 mm; 0mm<TH2≤0.5 mm; 0<PhiA/PhiD≤0.97; 0 mm<TH1+TH2≤1 mm; and0<2*(TH1+TH2)/PhiA≤0.5.

As shown in FIG. 1B to FIG. 1G, optical image capturing modulesaccording to a second structural embodiment to a seventh structuralembodiment are illustrated, each of which is slightly different fromthat of the first structural embodiment, but the effect ofminiaturization and high optical quality could be achieved as well.

The optical image capturing modules according to the second structuralembodiment is illustrated in FIG. 1B, which has almost the samestructure with that of the first structural embodiment, except that anouter peripheral wall of a lens barrel B2 has an external thread OT2thereon, and an inner wall of a lower through hole DH2 of a lens holderLH2 has an inner thread IT2 thereon, wherein the inner thread IT2 isadapted to be screwed with the external thread OT2, thereby to fix thelens barrel B2 in the lens holder LH2. In addition, an IR-cut filter IR2is fixed in the lens barrel B2 to filter out an excess infrared light.Moreover, the optical image capturing modules according to the secondstructural embodiment satisfies the conditions of the first structuralembodiment, which could keep small in size and provide high imagingquality as well.

The optical image capturing modules according to the third structuralembodiment is illustrated in FIG. 1C, which has almost the samestructure with that of the first structural embodiment, except that alens base LB3 is integrally formed as a monolithic unit, instead ofbeing separated to a lens barrel and a lens holder, which reduces thetime required for producing components and for assembling. In addition,an IR-cut filter IR3 is disposed in the lens base LB3. Moreover, amaximum value of a minimum length on a periphery of the lens base LB3perpendicular to an optical axis of the lens group L is denoted by PhiD.

Moreover, the optical image capturing modules according to the thirdstructural embodiment satisfies 0 mm<PhiA≤17.4 mm, and a preferablerange is 0 mm<PhiA≤13.5 mm; 0 mm<PhiD≤18 mm, and a preferable range is 0mm<PhiD≤15 mm; 0<PhiA/PhiD≤0.99, and a preferable range is0<PhiA/PhiD≤0.97; 0 mm<TH1+TH2≤1.5 mm, and a preferable range is 0mm<TH1+TH2≤1 mm; 0<2*(TH1+TH2)/PhiA≤0.95, and a preferable range is0<2*(TH1+TH2)/PhiA≤0.5. In other words, the optical image capturingmodules according to the third structural embodiment satisfies partiallyof the conditions of the first structural embodiment, which could keepsmall in size and provide high imaging quality as well.

The optical image capturing modules according to the fourth structuralembodiment is illustrated in FIG. 1D, which has almost the samestructure with that of the first structural embodiment, except that alens base LB4 includes a filter holder IRH4, a lens holder LH4, and alens barrel B4. The filter holder IRH4 has a through hole IH penetratingthrough both ends of the filter holder IRH4, and is disposed on thesensor holder SB. An IR-cut filter IR4 is disposed in the filter holderIRH4 and is located in the through hole IH of the filter holder IRH4, sothat the IR-cut filter IR4 is located above the image sensing componentS. The lens holder LH4 is fixed on the filter holder IRH4, and the lensbarrel B4 is disposed in the lens holder LH4, so that an upper throughhole UH4 of the lens barrel B4, a lower through hole DH4 of the lensholder LH4, and the through hole IH of the filter holder IRH4communicate with one another to form a receiving hole. In the currentembodiment, a glue is coated between the lens holder LH4 and the filterholder IRH4, and the lens holder LH4 and the filter holder IRH4 arefixed to each other via the glue, so that the lens holder LH4 is fixedon the filter holder IRH4. In addition, the optical image capturingmodules according to the fourth structural embodiment satisfies theconditions of the first structural embodiment, and could be fixed by aglue to carry out the active alignment assembly, which could keep smallin size and provide high imaging quality as well.

The optical image capturing modules according to the fifth structuralembodiment is illustrated in FIG. 1E, which has almost the samestructure with that of the fourth structural embodiment, except that anouter peripheral wall of a lens barrel B5 has an external thread OT5thereon, and an inner wall of a lower through hole DH5 of a lens holderLH5 has an inner thread IT5 thereon, wherein the inner thread IT5 isadapted to be screwed with the external thread OT5, thereby the lensbarrel B5 is dispose in the lens holder LH5 and is fixed in the lowerthrough hole DH5. In addition, the optical image capturing modulesaccording to the fifth structural embodiment satisfies the conditions ofthe first structural embodiment, which could keep small in size andprovide high imaging quality as well.

The optical image capturing modules according to the sixth structuralembodiment is illustrated in FIG. 1F, which has almost the samestructure with that of the first structural embodiment, except that anIR-cut filter IR6 is disposed on the sensor holder SB. In addition, theoptical image capturing module according to the sixth structuralembodiment satisfies the conditions of the first structural embodiment,which could keep small in size and provide high imaging quality as well.

The optical image capturing modules according to the seventh structuralembodiment is illustrated in FIG. 1G, which has almost the samestructure with that of the third structural embodiment, except that anIR-cut filter IR7 is disposed on the sensor holder SB. In addition, theoptical image capturing modules according to the seventh structuralembodiment satisfies the conditions of the first structural embodiment,which could keep small in size and provide high imaging quality as well.

Furthermore, the optical embodiments will be described in detail asfollow. The optical image capturing module could work in threewavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5nm is the main reference wavelength and is the reference wavelength forobtaining the technical characters. The optical image capturing modulecould also work in five wavelengths, including 470 nm, 510 nm, 555 nm,610 nm, and 650 nm wherein 555 nm is the main reference wavelength, andis the reference wavelength for obtaining the technical characters.

The optical image capturing module of the present invention satisfies0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, wherePPR is a ratio of the focal length f of the optical image capturingmodule to a focal length fp of each of lenses with positive refractivepower; NPR is a ratio of the focal length f of the optical imagecapturing module to a focal length fn of each of lenses with negativerefractive power; ΣPPR is a sum of the PPRs of each positive lens; andΣNPR is a sum of the NPRs of each negative lens. It is helpful forcontrol of an entire refractive power and an entire length of theoptical image capturing module.

The optical image capturing module further include an image sensorprovided on the image plane. The optical image capturing module of thepresent invention satisfies HOS/HOI≤50 and 0.5≤HOS/f≤150, and apreferable range is 1≤HOS/HOI≤40 and 1≤HOS/f≤140, where HOI is a half ofa diagonal of an effective sensing area of the image sensor, i.e., themaximum image height, and HOS is a height of the optical image capturingmodule, i.e. a distance on the optical axis between the object-sidesurface of the first lens and the image plane. It is helpful forreduction of the size of the optical image capturing module for used incompact cameras.

The optical image capturing module of the present invention further isprovided with an aperture to increase image quality.

In the optical image capturing module of the present invention, theaperture could be a front aperture or a middle aperture, wherein thefront aperture is provided between the object and the first lens, andthe middle is provided between the first lens and the image plane. Thefront aperture provides a long distance between an exit pupil of theoptical image capturing module and the image plane, which allows moreelements to be installed. The middle could enlarge a view angle of viewof the optical image capturing module and increase the efficiency of theimage sensor. The optical image capturing module satisfies0.1≤InS/HOS≤1.1, where InS is a distance between the aperture and theimage surface. It is helpful for size reduction and wide angle.

The optical image capturing module of the present invention satisfies0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-sidesurface of the first lens and the image-side surface of the sixth lens,and ETP is a sum of central thicknesses of the lenses on the opticalaxis. It is helpful for the contrast of image and yield rate ofmanufacture and provides a suitable back focal length for installationof other elements. In addition, the optical image capturing module ofthe present invention satisfies 0.1≤InTL/HOS≤0.95, which is helpful forreduction of the size of the optical image capturing module for used incompact cameras.

The optical image capturing system has a maximum image height HOI on theimage plane vertical to the optical axis. A transverse aberration at 0.7HOI in the positive direction of the tangential ray fan aberration afterthe longest operation wavelength of visible light passing through theedge of the entrance pupil is denoted by PLTA; a transverse aberrationat 0.7 HOI in the positive direction of the tangential ray fanaberration after the shortest operation wavelength of visible lightpassing through the edge of the entrance pupil is denoted by PSTA; atransverse aberration at 0.7 HOI in the negative direction of thetangential ray fan aberration after the longest operation wavelength ofvisible light passing through the edge of the entrance pupil is denotedby NLTA; a transverse aberration at 0.7 HOI in the negative direction ofthe tangential ray fan aberration after the shortest operationwavelength of visible light passing through the edge of the entrancepupil is denoted by NSTA; a transverse aberration at 0.7 HOI of thesagittal ray fan aberration after the longest operation wavelength ofvisible light passing through the edge of the entrance pupil is denotedby SLTA; a transverse aberration at 0.7 HOI of the sagittal ray fanaberration after the shortest operation wavelength of visible lightpassing through the edge of the entrance pupil is denoted by SSTA. Inaddition, the optical image capturing module has a better imageperformance when the optical image capturing module of the presentinvention satisfies PLTA≤100 μm; PSTA≤100 μm; NLTA≤100 μm; NSTA≤100 μm;SLTA≤100 μm; and SSTA≤100 μm.

The optical image capturing module of the present invention satisfies0.001≤|R1/R2|≤25, and a preferable range is 0.01≤|R1/R2|≤12, where R1 isa radius of curvature of the object-side surface of the first lens, andR2 is a radius of curvature of the image-side surface of the first lens.It provides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing module of the present invention satisfies−7<(R11−R12)/(R11+R12)<50, where R11 is a radius of curvature of theobject-side surface of the sixth lens, and R12 is a radius of curvatureof the image-side surface of the sixth lens. It may modify theastigmatic field curvature.

The optical image capturing module of the present invention satisfiesIN12/f≤60, where IN12 is a distance on the optical axis between thefirst lens and the second lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing module of the present invention satisfiesIN56/f≤3.0, where IN56 is a distance on the optical axis between thefifth lens and the sixth lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing module of the present invention satisfies0.1≤(TP1+IN12)/TP2≤10, where TP1 is a central thickness of the firstlens on the optical axis, and TP2 is a central thickness of the secondlens on the optical axis. It may control the sensitivity of manufactureof the optical image capturing module and improve the performance.

The optical image capturing module of the present invention satisfies0.1≤(TP6+IN56)/TP5≤15, where TP5 is a central thickness of the fifthlens on the optical axis, TP6 is a central thickness of the sixth lenson the optical axis, and IN56 is a distance between the fifth lens andthe sixth lens. It may control the sensitivity of manufacture of theoptical image capturing module and improve the performance.

The optical image capturing module of the present invention satisfies0.1≤TP4/(IN34+TP4+IN45)<1 where TP2 is a central thickness of the secondlens on the optical axis, TP3 is a central thickness of the third lenson the optical axis, TP4 is a central thickness of the fourth lens onthe optical axis, IN34 is a distance on the optical axis between thethird lens and the fourth lens, IN45 is a distance on the optical axisbetween the fourth lens and the fifth lens, and InTL is a distancebetween the object-side surface of the first lens and the image-sidesurface of the seventh lens. It may fine tune and correct the aberrationof the incident rays layer by layer, and reduce the height of theoptical image capturing module.

The optical image capturing module satisfies 0 mm≤HVT61≤3 mm; 0mm<HVT62≤6 mm; 0≤HVT61/HVT62; 0 mm≤|SGC61|≤0.5 mm; 0 mm<|SGC62|≤2 mm;and 0<|SGC62|/(|SGC62|+TP6)≤0.9, where HVT61 a distance perpendicular tothe optical axis between the critical point C61 on the object-sidesurface of the sixth lens and the optical axis; HVT62 a distanceperpendicular to the optical axis between the critical point C62 on theimage-side surface of the sixth lens and the optical axis; SGC61 is adistance on the optical axis between a point on the object-side surfaceof the sixth lens where the optical axis passes through and a pointwhere the critical point C61 projects on the optical axis; SGC62 is adistance on the optical axis between a point on the image-side surfaceof the sixth lens where the optical axis passes through and a pointwhere the critical point C62 projects on the optical axis. It is helpfulto correct the off-axis view field aberration.

The optical image capturing module satisfies 0.2≤HVT62/HOI≤0.9, andpreferably satisfies 0.3≤HVT62/HOI≤0.8. It may help to correct theperipheral aberration.

The optical image capturing module satisfies 0≤HVT62/HOS≤0.5, andpreferably satisfies 0.2≤HVT62/HOS≤0.45. It may help to correct theperipheral aberration.

The optical image capturing module of the present invention satisfies0<SGI611/(SGI611+TP6)≤0.9; 0<SGI621/(SGI621+TP6)≤0.9, and it ispreferable to satisfy 0.1≤SGI611/(SGI611+TP6)≤0.6;0.1≤SGI621/(SGI621+TP7)≤0.6, where SGI611 is a displacement on theoptical axis from a point on the object-side surface of the sixth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, projects on the optical axis, and SGI621 is a displacement on theoptical axis from a point on the image-side surface of the sixth lens,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface, which is the closest to the opticalaxis, projects on the optical axis.

The optical image capturing module of the present invention satisfies0<SGI612/(SGI612+TP6)≤0.9; 0<SGI622/(SGI622+TP6)≤0.9, and it ispreferable to satisfy 0.1≤SGI612/(SGI612+TP6)≤0.6;0.1≤SGI622/(SGI622+TP6)≤0.6, where SGI612 is a displacement on theoptical axis from a point on the object-side surface of the sixth lens,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, projects on the optical axis, and SGI622 is a displacementon the optical axis from a point on the image-side surface of the sixthlens, through which the optical axis passes, to a point where theinflection point on the object-side surface, which is the second closestto the optical axis, projects on the optical axis.

The optical image capturing module of the present invention satisfies0.001 mm≤|HIF611|≤5 mm; 0.001 mm≤|HIF621|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF611|≤3.5 mm; 1.5 mm≤|HIF621|≤3.5 mm, where HIF611 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens, which is the closestto the optical axis, and the optical axis; HIF621 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the sixth lens, which is the closest to theoptical axis, and the optical axis.

The optical image capturing module of the present invention satisfies0.001 mm≤|HIF612|≤5 mm; 0.001 mm≤|HIF622|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF622|≤3.5 mm; 0.1 mm≤|HIF612|≤3.5 mm, where HIF612 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens, which is the secondclosest to the optical axis, and the optical axis; HIF622 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the sixth lens, which is the second closest to theoptical axis, and the optical axis.

The optical image capturing module of the present invention satisfies0.001 mm≤|HIF613|≤5 mm; 0.001 mm≤|HIF623|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF623|≤3.5 mm; 0.1 mm≤|HIF613|≤3.5 mm, where HIF613 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens, which is the thirdclosest to the optical axis, and the optical axis; HIF623 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the sixth lens, which is the third closest to theoptical axis, and the optical axis.

The optical image capturing module of the present invention satisfies0.001 mm≤|HIF614|≤5 mm; 0.001 mm≤|HIF624|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF624|≤3.5 mm; 0.1 mm≤|HIF614|≤3.5 mm, where HIF614 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens, which is the fourthclosest to the optical axis, and the optical axis; HIF624 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the sixth lens, which is the fourth closest to theoptical axis, and the optical axis.

The optical image capturing module of the present invention satisfies0<(TH1+TH2)/HOI≤0.95; 0<(TH1+TH2)/HOS≤0.95; 0<2*(TH1+TH2)/PhiA≤0.95; andit is preferable to satisfy 0<(TH1+TH2)/HOI≤0.5; 0<(TH1+TH2)/HOS≤0.5;0<2*(TH1+TH2)/PhiA≤0.5.

In an embodiment, the lenses of high Abbe number and the lenses of lowAbbe number are arranged in an interlaced arrangement that could behelpful for correction of aberration of the optical image capturingmodule.

An equation of aspheric surface is

z=ch ²/[1+[1(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A6h ⁸ h+A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+  (1)

where z is a depression of the aspheric surface; k is conic constant; cis reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14,A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing module, the lenses could be made ofplastic or glass. The plastic lenses may reduce the weight and lower thecost of the optical image capturing module, and the glass lenses maycontrol the thermal effect and enlarge the space for arrangement of therefractive power of the optical image capturing module. In addition, theopposite surfaces (object-side surface and image-side surface) of thefirst to the seventh lenses could be aspheric that could obtain morecontrol parameters to reduce aberration. The number of aspheric glasslenses could be less than the conventional spherical glass lenses, whichis helpful for reduction of the height of the optical image capturingmodule.

When the lens has a convex surface, which means that the surface isconvex around a position, through which the optical axis passes, andwhen the lens has a concave surface, which means that the surface isconcave around a position, through which the optical axis passes.

The optical image capturing module of the present invention could beapplied in a dynamic focusing optical image capturing module. It issuperior in the correction of aberration and high imaging quality sothat it could be allied in lots of fields.

The optical image capturing module of the present invention couldfurther include a driving module to meet different demands, wherein thedriving module could be coupled with the lenses to move the lenses. Thedriving module could be a voice coil motor (VCM), which is used to movethe lens for focusing, or could be an optical image stabilization (OIS)component, which is used to lower the possibility of having the problemof image blurring which is caused by subtle movements of the lens whileshooting.

To meet different requirements, at least one lens among the first lensto the seventh lens of the optical image capturing module of the presentinvention could be a light filter, which filters out light of wavelengthshorter than 500 nm. Such effect could be achieved by coating on atleast one surface of the lens, or by using materials capable offiltering out short waves to make the lens.

To meet different requirements, the image plane of the optical imagecapturing module in the present invention could be either flat orcurved. If the image plane is curved (e.g., a sphere with a radius ofcurvature), the incidence angle required for focusing light on the imageplane could be decreased, which is not only helpful to shorten thelength of the optical image capturing module (TTL), but also helpful toincrease the relative illuminance.

We provide several optical embodiments in conjunction with theaccompanying drawings for the best understanding. In practice, theoptical embodiments of the present invention could be applied to otherstructural embodiments.

First Optical Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing module 10 ofthe first optical embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 110, anaperture 100, a second lens 120, a third lens 130, a fourth lens 140, afifth lens 150, a sixth lens 160, an IR-cut filter 180, an image plane190, and an image sensor 192.

The first lens 110 has negative refractive power and is made of plastic.An object-side surface 112 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 114 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 112 has two inflection points. A profile curve length of themaximum effective half diameter of the object-side surface 112 of thefirst lens 110 is denoted by ARS11, and a profile curve length of themaximum effective half diameter of the image-side surface 114 of thefirst lens 110 is denoted by ARS12. A profile curve length of a half ofthe entrance pupil diameter (HEP) of the object-side surface 112 of thefirst lens 110 is denoted by ARE11, and a profile curve length of a halfof the entrance pupil diameter (HEP) of the image-side surface 114 ofthe first lens 110 is denoted by ARE12. A thickness of the first lens110 on the optical axis is denoted by TP1.

The first lens satisfies SGI111=−0.0031 mm;|SGI111|/(|SGI111|+TP1)=0.0016, where a displacement on the optical axisfrom a point on the object-side surface 112 of the first lens 110,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface 112, which is the closest to theoptical axis, projects on the optical axis, is denoted by SGI111, and adisplacement on the optical axis from a point on the image-side surface114 of the first lens 110, through which the optical axis passes, to apoint where the inflection point on the image-side surface 114, which isthe closest to the optical axis, projects on the optical axis is denotedby SGI121.

The first lens 110 satisfies SGI112=1.3178 mm;|SGI112|/(|SGI112|+TP1)=0.4052, where a displacement on the optical axisfrom a point on the object-side surface 112 of the first lens 110,through which the optical axis passes, to a point where the inflectionpoint on the object-side surface 112, which is the second closest to theoptical axis, projects on the optical axis, is denoted by SGI112, and adisplacement on the optical axis from a point on the image-side surface114 of the first lens 110, through which the optical axis passes, to apoint where the inflection point on the image-side surface 114, which isthe second closest to the optical axis, projects on the optical axis isdenoted by SGI122.

The first lens 110 satisfies HIF111=0.5557 mm; HIF111/HOI=0.1111, wherea displacement perpendicular to the optical axis from a point on theobject-side surface 112 of the first lens 110, through which the opticalaxis passes, to the inflection point, which is the closest to theoptical axis is denoted by HIF111, and a displacement perpendicular tothe optical axis from a point on the image-side surface 114 of the firstlens 110, through which the optical axis passes, to the inflectionpoint, which is the closest to the optical axis is denoted by HIF121.

The first lens 110 satisfies HIF112=5.3732 mm; HIF112/HOI=1.0746, wherea displacement perpendicular to the optical axis from a point on theobject-side surface 112 of the first lens 110, through which the opticalaxis passes, to the inflection point, which is the second closest to theoptical axis is denoted by HIF112, and a displacement perpendicular tothe optical axis from a point on the image-side surface 114 of the firstlens 110, through which the optical axis passes, to the inflectionpoint, which is the second closest to the optical axis is denoted byHIF122.

The second lens 120 has positive refractive power and is made ofplastic. An object-side surface 122 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 124thereof, which faces the image side, is a convex aspheric surface. Theobject-side surface 122 has an inflection point. A profile curve lengthof the maximum effective half diameter of the object-side surface 122 ofthe second lens 120 is denoted by ARS21, and a profile curve length ofthe maximum effective half diameter of the image-side surface 124 of thesecond lens 120 is denoted by ARS22. A profile curve length of a half ofthe entrance pupil diameter (HEP) of the object-side surface 122 of thesecond lens 120 is denoted by ARE21, and a profile curve length of ahalf of the entrance pupil diameter (HEP) of the image-side surface 124of the second lens 120 is denoted by ARE22. A thickness of the secondlens 120 on the optical axis is denoted by TP2.

The second lens 120 satisfies SGI211=0.1069 mm;|SGI211|/(|SGI211|+TP2)=0.0412; SGI221=0 mm; |SGI221|/(|SGI221|+TP2)=0,where a displacement on the optical axis from a point on the object-sidesurface 122 of the second lens 120, through which the optical axispasses, to a point where the inflection point on the object-side surface122, which is the closest to the optical axis, projects on the opticalaxis, is denoted by SGI211, and a displacement on the optical axis froma point on the image-side surface 124 of the second lens 120, throughwhich the optical axis passes, to a point where the inflection point onthe image-side surface 124, which is the closest to the optical axis,projects on the optical axis is denoted by SGI221.

The second lens 120 satisfies HIF211=1.1264 mm; HIF211/HOI=0.2253;HIF221=0 mm; HIF221/HOI=0, where a displacement perpendicular to theoptical axis from a point on the object-side surface 122 of the secondlens 120, through which the optical axis passes, to the inflectionpoint, which is the closest to the optical axis is denoted by HIF211,and a displacement perpendicular to the optical axis from a point on theimage-side surface 124 of the second lens 120, through which the opticalaxis passes, to the inflection point, which is the closest to theoptical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic.An object-side surface 132, which faces the object side, is a concaveaspheric surface, and an image-side surface 134, which faces the imageside, is a convex aspheric surface. The object-side surface 132 has aninflection point, and the image-side surface 134 has an inflectionpoint. The object-side surface 122 has an inflection point. A profilecurve length of the maximum effective half diameter of the object-sidesurface 132 of the third lens 130 is denoted by ARS31, and a profilecurve length of the maximum effective half diameter of the image-sidesurface 134 of the third lens 130 is denoted by ARS32. A profile curvelength of a half of the entrance pupil diameter (HEP) of the object-sidesurface 132 of the third lens 130 is denoted by ARE31, and a profilecurve length of a half of the entrance pupil diameter (HEP) of theimage-side surface 134 of the third lens 130 is denoted by ARE32. Athickness of the third lens 130 on the optical axis is denoted by TP3.

The third lens 130 satisfies SGI311=−0.3041 mm;|SGI311|/(|SGI311|+TP3)=0.4445; SGI321=−0.1172 mm;|SGI321|/(|SGI321|+TP3)=0.2357, where SGI311 is a displacement on theoptical axis from a point on the object-side surface 132 of the thirdlens 130, through which the optical axis passes, to a point where theinflection point on the object-side surface 132, which is the closest tothe optical axis, projects on the optical axis, and SGI321 is adisplacement on the optical axis from a point on the image-side surface134 of the third lens 130, through which the optical axis passes, to apoint where the inflection point on the image-side surface 134, which isthe closest to the optical axis, projects on the optical axis.

The third lens 130 satisfies HIF311=1.5907 mm; HIF311/HOI=0.3181;HIF321=1.3380 mm; HIF321/HOI=0.2676, where HIF311 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface 132 of the third lens 130, which is the closest tothe optical axis, and the optical axis; HIF321 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface 134 of the third lens 130, which is the closest tothe optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made ofplastic. An object-side surface 142, which faces the object side, is aconvex aspheric surface, and an image-side surface 144, which faces theimage side, is a concave aspheric surface. The object-side surface 142has two inflection points, and the image-side surface 144 has aninflection point. A profile curve length of the maximum effective halfdiameter of the object-side surface 142 of the fourth lens 140 isdenoted by ARS41, and a profile curve length of the maximum effectivehalf diameter of the image-side surface 144 of the fourth lens 140 isdenoted by ARS42. A profile curve length of a half of the entrance pupildiameter (HEP) of the object-side surface 142 of the fourth lens 140 isdenoted by ARE41, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface 144 of the fourth lens140 is denoted by ARE42. A thickness of the fourth lens 140 on theoptical axis is TP4.

The fourth lens 140 satisfies SGI411=0.0070 mm;|SGI411|/(|SGI411|+TP4)=0.0056; SGI421=0.0006 mm;|SGI421|/(|SGI421|+TP4)=0.0005, where SGI411 is a displacement on theoptical axis from a point on the object-side surface 142 of the fourthlens 140, through which the optical axis passes, to a point where theinflection point on the object-side surface 142, which is the closest tothe optical axis, projects on the optical axis, and SGI421 is adisplacement on the optical axis from a point on the image-side surface144 of the fourth lens 140, through which the optical axis passes, to apoint where the inflection point on the image-side surface 144, which isthe closest to the optical axis, projects on the optical axis.

The fourth lens 140 satisfies SGI412=−0.2078 mm;|SGI412|/(|SGI412|+TP4)=0.1439, where SGI412 is a displacement on theoptical axis from a point on the object-side surface 142 of the fourthlens 140, through which the optical axis passes, to a point where theinflection point on the object-side surface 142, which is the secondclosest to the optical axis, projects on the optical axis, and SGI422 isa displacement on the optical axis from a point on the image-sidesurface 144 of the fourth lens 140, through which the optical axispasses, to a point where the inflection point on the image-side surface144, which is the second closest to the optical axis, projects on theoptical axis.

The fourth lens 140 further satisfies HIF411=0.4706 mm;HIF411/HOI=0.0941; HIF421=0.1721 mm; HIF421/HOI=0.0344, where HIF411 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface 142 of the fourth lens 140, which isthe closest to the optical axis, and the optical axis; HIF421 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface 144 of the fourth lens 140, which is theclosest to the optical axis, and the optical axis.

The fourth lens 140 satisfies HIF412=2.0421 mm; HIF412/HOI=0.4084, whereHIF412 is a distance perpendicular to the optical axis between theinflection point on the object-side surface 142 of the fourth lens 140,which is the second closest to the optical axis, and the optical axis;HIF422 is a distance perpendicular to the optical axis between theinflection point on the image-side surface 144 of the fourth lens 140,which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic.An object-side surface 152, which faces the object side, is a convexaspheric surface, and an image-side surface 154, which faces the imageside, is a convex aspheric surface. The object-side surface 152 has twoinflection points, and the image-side surface 154 has an inflectionpoint. A profile curve length of the maximum effective half diameter ofthe object-side surface 152 of the fifth lens 150 is denoted by ARS51,and a profile curve length of the maximum effective half diameter of theimage-side surface 154 of the fifth lens 150 is denoted by ARS52. Aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe object-side surface 152 of the fifth lens 150 is denoted by ARE51,and a profile curve length of a half of the entrance pupil diameter(HEP) of the image-side surface 154 of the fifth lens 150 is denoted byARE52. A thickness of the fifth lens 150 on the optical axis is denotedby TP5.

The fifth lens 150 satisfies SGI511=0.00364 mm; SGI521=−0.63365 mm;|SGI511|/(|SGI511|+TP5)=0.00338; |SGI521|/(|SGI521|+TP5)=0.37154, whereSGI511 is a displacement on the optical axis from a point on theobject-side surface 152 of the fifth lens 150, through which the opticalaxis passes, to a point where the inflection point on the object-sidesurface 152, which is the closest to the optical axis, projects on theoptical axis, and SGI521 is a displacement on the optical axis from apoint on the image-side surface 154 of the fifth lens 150, through whichthe optical axis passes, to a point where the inflection point on theimage-side surface 154, which is the closest to the optical axis,projects on the optical axis.

The fifth lens 150 satisfies SGI512=−0.32032 mm;|SGI512|/(|SGI512|+TP5)=0.23009, where SGI512 is a displacement on theoptical axis from a point on the object-side surface 152 of the fifthlens 150, through which the optical axis passes, to a point where theinflection point on the object-side surface 152, which is the secondclosest to the optical axis, projects on the optical axis, and SGI522 isa displacement on the optical axis from a point on the image-sidesurface 154 of the fifth lens 150, through which the optical axispasses, to a point where the inflection point on the image-side surface154, which is the second closest to the optical axis, projects on theoptical axis.

The fifth lens 150 satisfies SGI513=0 mm; SGI523=0 mm;|SGI513|/(|SGI513|+TP5)=0; |SGI523|/(|SGI523|+TP5)=0, where SGI513 is adisplacement on the optical axis from a point on the object-side surface152 of the fifth lens 150, through which the optical axis passes, to apoint where the inflection point on the object-side surface 152, whichis the third closest to the optical axis, projects on the optical axis,and SGI523 is a displacement on the optical axis from a point on theimage-side surface 154 of the fifth lens 150, through which the opticalaxis passes, to a point where the inflection point on the image-sidesurface 154, which is the third closest to the optical axis, projects onthe optical axis.

The fifth lens 150 satisfies SGI514=0 mm; SGI524=0 mm;|SGI514|/(|SGI514|+TP5)=0; |SGI524|/(|SGI524|+TP5)=0, where SGI514 is adisplacement on the optical axis from a point on the object-side surface152 of the fifth lens 150, through which the optical axis passes, to apoint where the inflection point on the object-side surface 152, whichis the fourth closest to the optical axis, projects on the optical axis,and SGI524 is a displacement on the optical axis from a point on theimage-side surface 154 of the fifth lens 150, through which the opticalaxis passes, to a point where the inflection point on the image-sidesurface 154, which is the fourth closest to the optical axis, projectson the optical axis.

The fifth lens 150 further satisfies HIF511=0.28212 mm; HIF521=2.13850mm; HIF511/HOI=0.05642; HIF521/HOI=0.42770, where HIF511 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface 152 of the fifth lens 150, which is the closest tothe optical axis, and the optical axis; HIF521 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface 154 of the fifth lens 150, which is the closest tothe optical axis, and the optical axis.

The fifth lens 150 further satisfies HIF512=2.51384 mm;HIF512/HOI=0.50277, where HIF512 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 152of the fifth lens 150, which is the second closest to the optical axis,and the optical axis; HIF522 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 154 of thefifth lens 150, which is the second closest to the optical axis, and theoptical axis.

The fifth lens 150 further satisfies HIF513=0 mm; HIF513/HOI=0; HIF523=0mm; HIF523/HOI=0, where HIF513 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 152of the fifth lens 150, which is the third closest to the optical axis,and the optical axis; HIF523 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 154 of thefifth lens 150, which is the third closest to the optical axis, and theoptical axis.

The fifth lens 150 further satisfies HIF514=0 mm; HIF514/HOI=0; HIF524=0mm; HIF524/HOI=0, where HIF514 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 152of the fifth lens 150, which is the fourth closest to the optical axis,and the optical axis; HIF524 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 154 of thefifth lens 150, which is the fourth closest to the optical axis, and theoptical axis.

The sixth lens 160 has negative refractive power and is made of plastic.An object-side surface 162, which faces the object side, is a concavesurface, and an image-side surface 164, which faces the image side, is aconcave surface. The object-side surface 162 has two inflection points,and the image-side surface 164 has an inflection point. Whereby, theincident angle of each view field entering the sixth lens 160 could beeffectively adjusted to improve aberration. A profile curve length ofthe maximum effective half diameter of the object-side surface 162 ofthe sixth lens 160 is denoted by ARS61, and a profile curve length ofthe maximum effective half diameter of the image-side surface 164 of thesixth lens 160 is denoted by ARS62. A profile curve length of a half ofthe entrance pupil diameter (HEP) of the object-side surface 162 of thesixth lens 160 is denoted by ARE61, and a profile curve length of a halfof the entrance pupil diameter (HEP) of the image-side surface 164 ofthe sixth lens 160 is denoted by ARE62. A thickness of the sixth lens160 on the optical axis is denoted by TP6.

The sixth lens 160 satisfies SGI611=−0.38558 mm; SGI621=0.12386 mm;|SGI611|/(|SGI611|+TP6)=0.27212; |SGI621|/(|SGI621|+TP6)=0.10722, whereSGI611 is a displacement on the optical axis from a point on theobject-side surface 162 of the sixth lens 160, through which the opticalaxis passes, to a point where the inflection point on the object-sidesurface 162, which is the closest to the optical axis, projects on theoptical axis, and SGI621 is a displacement on the optical axis from apoint on the image-side surface 164 of the sixth lens 160, through whichthe optical axis passes, to a point where the inflection point on theimage-side surface 164, which is the closest to the optical axis,projects on the optical axis.

The sixth lens 160 satisfies SGI612=−0.47400 mm;|SGI612|/(|SGI612|+TP6)=0.31488; SGI622=0 mm; |SGI6221/(|SGI6221+TP6)=0,where SGI612 is a displacement on the optical axis from a point on theobject-side surface 162 of the sixth lens 160, through which the opticalaxis passes, to a point where the inflection point on the object-sidesurface 162, which is the second closest to the optical axis, projectson the optical axis, and SGI622 is a displacement on the optical axisfrom a point on the image-side surface 164 of the sixth lens 160,through which the optical axis passes, to a point where the inflectionpoint on the image-side surface 164, which is the second closest to theoptical axis, projects on the optical axis.

The sixth lens 160 further satisfies HIF611=2.24283 mm; HIF621=1.07376mm; HIF611/HOI=0.44857; HIF621/HOI=0.21475, where HIF611 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface 162 of the sixth lens 160, which is the closest tothe optical axis, and the optical axis; HIF621 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface 164 of the sixth lens 160, which is the closest tothe optical axis, and the optical axis.

The sixth lens 160 further satisfies HIF612=2.48895 mm;HIF612/HOI=0.49779, where HIF612 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 162of the sixth lens 160, which is the second closest to the optical axis,and the optical axis; HIF622 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 164 of thesixth lens 160, which is the second closest to the optical axis, and theoptical axis.

The sixth lens 160 further satisfies HIF613=0 mm; HIF613/HOI=0; HIF623=0mm; HIF623/HOI=0, where HIF613 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 162of the sixth lens 160, which is the third closest to the optical axis,and the optical axis; HIF623 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 164 of thesixth lens 160, which is the third closest to the optical axis, and theoptical axis.

The sixth lens 160 further satisfies HIF614=0 mm; HIF614/HOI=0; HIF624=0mm; HIF624/HOI=0, where HIF614 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface 162of the sixth lens 160, which is the fourth closest to the optical axis,and the optical axis; HIF624 is a distance perpendicular to the opticalaxis between the inflection point on the image-side surface 164 of thesixth lens 160, which is the fourth closest to the optical axis, and theoptical axis.

The IR-cut filter 180 is made of glass and is disposed between the sixthlens 160 and the image plane 190. The IR-cut filter 180 gives nocontribution to the focal length of the optical image capturing module.

The optical image capturing module 10 of the first optical embodimenthas the following parameters, which are f=4.075 mm; f/HEP=1.4;HAF=50.001 degrees; and tan(HAF)=1.1918, where f is a focal length ofthe lens group; HAF is a half of the maximum field angle; and HEP is anentrance pupil diameter.

The parameters of the lenses of the first optical embodiment aref1=−7.828 mm; |f/f1|=0.52060; f6=−4.886; and |f1|>f6, where f1 is afocal length of the first lens 110; and f6 is a focal length of thesixth lens 160.

The first optical embodiment further satisfies|f2|+|f3|+|f4|+|f5|=95.50815; |f1|+|f6|=12.71352 and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|, where f2 is a focal length of the secondlens 120, f3 is a focal length of the third lens 130, f4 is a focallength of the fourth lens 140, f5 is a focal length of the fifth lens150, and f6 is a focal length of the sixth lens 160.

The optical image capturing module 10 of the first optical embodimentfurther satisfies ΣPPR=f/f2+f/f4+f/f5=1.63290;ΣNPR=|f/f1|+|f/f3|+|f/f6|=1.51305; ΣPPR/|ΣNPR|=1.07921; |f/f2|=0.69101;|f/f3|=0.15834; |f/f4|=0.06883; |f/f5|=0.87305; and |f/f6|=0.83412,where PPR is a ratio of a focal length f of the optical image capturingmodule to a focal length fp of each of the lenses with positiverefractive power; and NPR is a ratio of a focal length f of the opticalimage capturing module to a focal length fn of each of lenses withnegative refractive power.

The optical image capturing module 10 of the first optical embodimentfurther satisfies InTL+BFL=HOS; HOS=19.54120 mm; HOI=5.0 mm;HOS/HOI=3.90824; HOS/f=4.7952; InS=11.685 mm; InTL/HOS=0.9171; andInS/HOS=0.59794, where InTL is a distance between the object-sidesurface 112 of the first lens 110 and the image-side surface 164 of thesixth lens 160; HOS is a height of the image capturing system, i.e. adistance between the object-side surface 112 of the first lens 110 andthe image plane 190; InS is a distance between the aperture 100 and theimage plane 190; HOI is a half of a diagonal of an effective sensingarea of the image sensor 192, i.e., the maximum image height; and BFL isa distance between the image-side surface 164 of the sixth lens 160 andthe image plane 190.

The optical image capturing module 10 of the first optical embodimentfurther satisfies ΣTP=8.13899 mm; and ΣTP/InTL=0.52477, where ΣTP is asum of the thicknesses of the lenses 110-160 with refractive power. Itis helpful for the contrast of image and yield rate of manufacture andprovides a suitable back focal length for installation of otherelements.

The optical image capturing module 10 of the first optical embodimentfurther satisfies |R1/R2|=129.9952, where R1 is a radius of curvature ofthe object-side surface 112 of the first lens 110, and R2 is a radius ofcurvature of the image-side surface 114 of the first lens 110. Itprovides the first lens 110 with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing module 10 of the first optical embodimentfurther satisfies (R11−R12)/(R11+R12)=1.27780, where R11 is a radius ofcurvature of the object-side surface 162 of the sixth lens 160, and R12is a radius of curvature of the image-side surface 164 of the sixth lens160. It may modify the astigmatic field curvature.

The optical image capturing module 10 of the first optical embodimentfurther satisfies ΣPP=f2+f4+f5=69.770 mm; and f5/(f2+f4+f5)=0.067, whereΣPP is a sum of the focal lengths fp of each lens with positiverefractive power. It is helpful to share the positive refractive powerof a single lens to other positive lenses to avoid the significantaberration caused by the incident rays.

The optical image capturing module 10 of the first optical embodimentfurther satisfies ΣNP=f1+f3+f6=−38.451 mm; and f6/(f1+f3+f6)=0.127,where ΣNP is a sum of the focal lengths fn of each lens with negativerefractive power. It is helpful to share the negative refractive powerof the sixth lens 160 to the other negative lens, which avoid thesignificant aberration caused by the incident rays.

The optical image capturing module 10 of the first optical embodimentfurther satisfies IN12=6.418 mm; IN12/f=1.57491, where IN12 is adistance on the optical axis between the first lens 110 and the secondlens 120. It may correct chromatic aberration and improve theperformance.

The optical image capturing module 10 of the first optical embodimentfurther satisfies IN56=0.025 mm; IN56/f=0.00613, where IN56 is adistance on the optical axis between the fifth lens 150 and the sixthlens 160. It may correct chromatic aberration and improve theperformance.

The optical image capturing module 10 of the first optical embodimentfurther satisfies TP1=1.934 mm; TP2=2.486 mm; and(TP1+IN12)/TP2=3.36005, where TP1 is a central thickness of the firstlens 110 on the optical axis, and TP2 is a central thickness of thesecond lens 120 on the optical axis. It may control the sensitivity ofmanufacture of the optical image capturing module and improve theperformance.

The optical image capturing module 10 of the first optical embodimentfurther satisfies TP5=1.072 mm; TP6=1.031 mm; and(TP6+IN56)/TP5=0.98555, where TP5 is a central thickness of the fifthlens 150 on the optical axis, TP6 is a central thickness of the sixthlens 160 on the optical axis, and IN56 is a distance on the optical axisbetween the fifth lens 150 and the sixth lens 160. It may control thesensitivity of manufacture of the optical image capturing module andlower the total height of the optical image capturing module.

The optical image capturing module 10 of the first optical embodimentfurther satisfies IN34⁼0.401 mm; IN45=0.025 mm; andTP4/(IN34+TP4+IN45)=0.74376, where TP4 is a central thickness of thefourth lens 140 on the optical axis; IN34 is a distance on the opticalaxis between the third lens 130 and the fourth lens 140; 1N45 is adistance on the optical axis between the fourth lens 140 and the fifthlens 150. It may help to slightly correct the aberration caused by theincident rays and lower the total height of the optical image capturingmodule.

The optical image capturing module 10 of the first optical embodimentfurther satisfies InRS51=−0.34789 mm; InRS52=−0.88185 mm;|InRS51|/TP5=0.32458; and |InRS52|/TP5=0.82276, where InRS51 is adisplacement from a point on the object-side surface 152 of the fifthlens 150 passed through by the optical axis to a point on the opticalaxis where a projection of the maximum effective semi diameter of theobject-side surface 152 of the fifth lens 150 ends; InRS52 is adisplacement from a point on the image-side surface 154 of the fifthlens 150 passed through by the optical axis to a point on the opticalaxis where a projection of the maximum effective semi diameter of theimage-side surface 154 of the fifth lens 150 ends; and TP5 is a centralthickness of the fifth lens 150 on the optical axis. It is helpful formanufacturing and shaping of the lenses and is helpful to reduce thesize.

The optical image capturing module 10 of the first optical embodimentfurther satisfies HVT51=0.515349 mm; and HVT52=0 mm, where HVT51 is adistance perpendicular to the optical axis between the critical point onthe object-side surface 152 of the fifth lens 150 and the optical axis;and HVT52 is a distance perpendicular to the optical axis between thecritical point on the image-side surface 154 of the fifth lens 150 andthe optical axis.

The optical image capturing module 10 of the first optical embodimentfurther satisfies InRS61=−0.58390 mm; InRS62=0.41976 mm;|InRS61|/TP6=0.56616; and |InRS62|/TP6=0.40700, where InRS61 is adisplacement from a point on the object-side surface 162 of the sixthlens 160 passed through by the optical axis to a point on the opticalaxis where a projection of the maximum effective semi diameter of theobject-side surface 162 of the sixth lens 160 ends; InRS62 is adisplacement from a point on the image-side surface 164 of the sixthlens 160 passed through by the optical axis to a point on the opticalaxis where a projection of the maximum effective semi diameter of theimage-side surface 164 of the sixth lens 160 ends; and TP6 is a centralthickness of the sixth lens 160 on the optical axis. It is helpful formanufacturing and shaping of the lenses and is helpful to reduce thesize.

The optical image capturing module 10 of the first optical embodimentsatisfies HVT61=0 mm; and HVT62=0 mm, where HVT61 is a distanceperpendicular to the optical axis between the critical point on theobject-side surface 162 of the sixth lens 160 and the optical axis; andHVT62 is a distance perpendicular to the optical axis between thecritical point on the image-side surface 164 of the sixth lens 160 andthe optical axis.

The optical image capturing module 10 of the first optical embodimentsatisfies HVT51/HOI=0.1031. It is helpful for correction of theaberration of the peripheral view field of the optical image capturingmodule.

The optical image capturing module 10 of the first optical embodimentsatisfies HVT51/HOS=0.02634. It is helpful for correction of theaberration of the peripheral view field of the optical image capturingmodule.

The second lens 120, the third lens 130, and the sixth lens 160 havenegative refractive power. The optical image capturing module 10 of thefirst optical embodiment further satisfies NA6/NA2≤1, where NA2 is anAbbe number of the second lens 120; NA3 is an Abbe number of the thirdlens 130; and NA6 is an Abbe number of the sixth lens 160. It maycorrect the aberration of the optical image capturing module.

The optical image capturing module 10 of the first optical embodimentfurther satisfies |TDT|=2.124%; |ODT|=5.076%, where TDT is TVdistortion; and ODT is optical distortion.

The optical image capturing module 10 of the first optical embodimentfurther satisfies LS=12 mm; PhiA=2*(EHD62)=6.726 mm;PhiC=PhiA+2*TH2=7.026 mm; PhiD=PhiC+2*(TH1+TH2)=7.426 mm; TH1=0.2 mm;TH2=0.15 mm; PhiA/PhiD=0.9057; TH1+TH2=0.35 mm; (TH1+TH2)/HOI=0.035;(TH1+TH2)/HOS=0.0179; 2(TH1+TH2)/PhiA=0.1041; (TH1+TH2)/LS=0.0292, whereEHD62 is a maximum effective half diameter of the image-side surface 164of the sixth lens 160.

The parameters of the lenses of the first optical embodiment are listedin Table 1 and Table 2.

TABLE 1 f = 4.075 mm; f/HEP = 1.4; HAF = 50.000 deg Focal ThicknessRefractive Abbe length Surface Radius of curvature (mm) (mm) Materialindex number (mm) 0 Object plane plane 1 1^(st) lens −40.99625704 1.934plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Aperture plane 0.495 42^(nd) lens 5.333427366 2.486 plastic 1.544 55.96 5.897 5 −6.7816599710.502 6 3^(rd) lens −5.697794287 0.380 plastic 1.642 22.46 −25.738 7−8.883957518 0.401 8 4^(th) lens 13.19225664 1.236 plastic 1.544 55.9659.205 9 21.55681832 0.025 10 5^(th) lens 8.987806345 1.072 plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 6^(th) lens −29.464914251.031 plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 Infrared plane0.200 1.517 64.13 rays filter 15 plane 1.420 16 Image plane planeReference wavelength (d-line): 555 mm; the position of blocking light:the effective half diameter of the clear aperture of the first surfaceis 5.800 mm; the effective diameter of the clear aperture of the thirdsurface is 1.570 mm; the effective diameter of the clear aperture of thefifth surface is 1.950 mm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k4.310876E+01 −4.707622E+00 2.616025E+00 2.445397E+00 5.645686E+00−2.117147E+01 −5.287220E+00 A4 7.054243E−03 1.714312E−02 −8.377541E−03−1.789549E−02 −3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04−1.502232E−04 −1.838068E−03 −3.657520E−03 −1.225453E−03 6.250200E−032.743532E−03 A8 3.077890E−05 −1.359611E−04 1.233332E−03 −1.131622E−03−5.979572E−03 −5.854426E−03 −2.457574E−03 A10 −1.260650E−06 2.680747E−05−2.390895E−03 1.390351E−03 4.556449E−03 4.049451E−03 1.874319E−03 A123.319093E−08 −2.017491E−06 1.998555E−03 −4.152857E−04 −1.177175E−03−1.314592E−03 −6.013661E−04 A14 −5.051600E−10 6.604615E−08 −9.734019E−045.487286E−05 1.370522E−04 2.143097E−04 8.792480E−05 A16 3.380000E−12−1.301630E−09 2.478373E−04 −2.919339E−06 −5.974015E−06 −1.399894E−05−4.770527E−06 Surface 9 10 11 12 13 k 6.200000E+01 −2.114008E+01−7.699904E+00 −6.155476E+01 −3.120467E−01 A4 −1.359965E−01 −1.263831E−01−1.927804E−02 −2.492467E−02 −3.521844E−02 A6 6.628518E−02 6.965399E−022.478376E−03 −1.835360E−03 5.629654E−03 A8 −2.129167E−02 −2.116027E−021.438785E−03 3.201343E−03 −5.466925E−04 A10 4.396344E−03 3.819371E−03−7.013749E−04 −8.990757E−04 2.231154E−05 A12 −5.542899E−04 −4.040283E−041.253214E−04 1.245343E−04 5.548990E−07 A14 3.768879E−05 2.280473E−05−9.943196E−06 −8.788363E−06 −9.396920E−08 A16 −1.052467E−06−5.165452E−07 2.898397E−07 2.494302E−07 2.728360E−09

The figures related to the profile curve lengths obtained based on Table1 and Table 2 are listed in the following table:

First optical embodiment (Reference wavelength (d-line): 555 mm) ARE ARE− 2(ARE/HEP) ARE/TP ARE 1/2(HEP) value 1/2(HEP) % TP (%) 11 1.455 1.455−0.00033  99.98% 1.934 75.23% 12 1.455 1.495 0.03957 102.72% 1.93477.29% 21 1.455 1.465 0.00940 100.65% 2.486 58.93% 22 1.455 1.4950.03950 102.71% 2.486 60.14% 31 1.455 1.486 0.03045 102.09% 0.380391.02% 32 1.455 1.464 0.00830 100.57% 0.380 385.19% 41 1.455 1.4580.00237 100.16% 1.236 117.95% 42 1.455 1.484 0.02825 101.94% 1.236120.04% 51 1.455 1.462 0.00672 100.46% 1.072 136.42% 52 1.455 1.4990.04335 102.98% 1.072 139.83% 61 1.455 1.465 0.00964 100.66% 1.031142.06% 62 1.455 1.469 0.01374 100.94% 1.031 142.45% ARS (ARS/EHD)ARS/TP ARS EHD value ARS − EHD % TP (%) 11 5.800 6.141 0.341 105.88%1.934 317.51% 12 3.299 4.423 1.125 134.10% 1.934 228.70% 21 1.664 1.6740.010 100.61% 2.486 67.35% 22 1.950 2.119 0.169 108.65% 2.486 85.23% 311.980 2.048 0.069 103.47% 0.380 539.05% 32 2.084 2.101 0.017 100.83%0.380 552.87% 41 2.247 2.287 0.040 101.80% 1.236 185.05% 42 2.530 2.8130.284 111.22% 1.236 227.63% 51 2.655 2.690 0.035 101.32% 1.072 250.99%52 2.764 2.930 0.166 106.00% 1.072 273.40% 61 2.816 2.905 0.089 103.16%1.031 281.64% 62 3.363 3.391 0.029 100.86% 1.031 328.83%

The detail parameters of the first optical embodiment are listed inTable 1, in which the unit of the radius of curvature, thickness, andfocal length are millimeter, and surface 0-16 indicates the surfaces ofall elements in the system in sequence from the object side to the imageside. Table 2 is the list of coefficients of the aspheric surfaces, inwhich k indicates the taper coefficient in the aspheric curve equation,and A1-A20 indicate the coefficients of aspheric surfaces from the firstorder to the twentieth order of each aspheric surface. The followingoptical embodiments have the similar diagrams and tables, which are thesame as those of the first optical embodiment, so we do not describe itagain. The definitions of the mechanism component parameters of thefollowing optical embodiments are the same as those of the first opticalembodiment.

Second Optical Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing module 20 ofthe second optical embodiment of the present invention includes, alongan optical axis from an object side to an image side, a first lens 210,a second lens 220, a third lens 230, an aperture 200, a fourth lens 240,a fifth lens 250, a sixth lens 260, a seventh lens 270, an IR-cut filter280, an image plane 290, and an image sensor 292.

The first lens 210 has negative refractive power and is made of glass.An object-side surface 212 thereof, which faces the object side, is aconvex spherical surface, and an image-side surface 214 thereof, whichfaces the image side, is a concave spherical surface.

The second lens 220 has negative refractive power and is made of glass.An object-side surface 222 thereof, which faces the object side, is aconcave spherical surface, and an image-side surface 224 thereof, whichfaces the image side, is a convex spherical surface.

The third lens 230 has positive refractive power and is made of glass.An object-side surface 232, which faces the object side, is a convexspherical surface, and an image-side surface 234, which faces the imageside, is a convex spherical surface.

The fourth lens 240 has positive refractive power and is made of glass.An object-side surface 242, which faces the object side, is a convexspherical surface, and an image-side surface 244, which faces the imageside, is a convex spherical surface.

The fifth lens 250 has positive refractive power and is made of glass.An object-side surface 252, which faces the object side, is a convexspherical surface, and an image-side surface 254, which faces the imageside, is a convex spherical surface.

The sixth lens 260 has negative refractive power and is made of glass.An object-side surface 262, which faces the object side, is a concavespherical surface, and an image-side surface 264, which faces the imageside, is a concave spherical surface. Whereby, the incident angle ofeach view field entering the sixth lens 260 could be effectivelyadjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made of glass.An object-side surface 272, which faces the object side, is a convexsurface, and an image-side surface 274, which faces the image side, is aconvex surface. It may help to shorten the back focal length to keepsmall in size, and may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The IR-cut filter 280 is made of glass and is disposed between theseventh lens 270 and the image plane 290. The IR-cut filter 280 gives nocontribution to the focal length of the optical image capturing module.

The parameters of the lenses of the second optical embodiment are listedin Table 3 and Table 4.

TABLE 3 f = 4.7601 mm; f/HEP = 2.2; HAF = 95.98 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 47.71478323 4.977glass 2.001 29.13 −12.647 2 9.527614761 13.737 3 2^(nd) lens−14.88061107 5.000 glass 2.001 29.13 −99.541 4 −20.42046946 10.837 53^(rd) lens 182.4762997 5.000 glass 1.847 23.78 44.046 6 −46.7196360813.902 7 Aperture 1E+18 0.850 8 4^(th) lens 28.60018103 4.095 glass1.834 37.35 19.369 9 −35.08507586 0.323 10 5^(th) lens 18.25991342 1.539glass 1.609 46.44 20.223 11 −36.99028878 0.546 12 6^(th) lens−18.24574524 5.000 glass 2.002 19.32 −7.668 13 15.33897192 0.215 147^(th) lens 16.13218937 4.933 glass 1.517 64.20 13.620 15 −11.240078.664 16 Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.00718 Image 1E+18 −0.007 plane Reference wavelength (d-line): 555 nm

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A80.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00

An equation of the aspheric surfaces of the second optical embodiment isthe same as that of the first optical embodiment, and the definitionsare the same as well.

The exact parameters of the second optical embodiment based on Table 3and Table 4 are listed in the following table:

Second optical embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.3764 0.0478 0.1081 0.2458 0.2354 0.6208|f/f7| Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN67/f 0.3495 1.3510 0.63272.1352 2.8858 0.0451 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP60.1271 2.2599 3.7428 1.0296 HOS InTL HOS/HOI InS/HOS ODT % TDT % 81.617870.9539 13.6030 0.3451 −113.2790 84.4806 HVT11 HVT12 HVT21 HVT22 HVT31HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PhiA PhiCPhiD TH1 TH2 HOI 11.962 mm 12.362 mm 12.862 mm 0.25 mm 0.2 mm 6 mm(TH1 + TH2)/ (TH1 + TH2)/ 2(TH1 + TH2)/ PhiA/PhiD TH1 + TH2 HOI HOS PhiAInTL/HOS 0.9676 0.45 mm 0.075 0.0055 0.0752 0.8693 PSTA PLTA NSTA NLTASSTA SLTA 0.060 mm −0.005 mm 0.016 mm 0.006 mm 0.020 mm −0.008 mm

The figures related to the profile curve lengths obtained based on Table3 and Table 4 are listed in the following table:

Second optical embodiment (Reference wavelength: 555 nm) ARE ARE −2(ARE/HEP) ARE/TP ARE 1/2(HEP) value 1/2(HEP) % TP (%) 11 1.082 1.081−0.00075 99.93% 4.977 21.72% 12 1.082 1.083 0.00149 100.14% 4.977 21.77%21 1.082 1.082 0.00011 100.01% 5.000 21.64% 22 1.082 1.082 −0.0003499.97% 5.000 21.63% 31 1.082 1.081 −0.00084 99.92% 5.000 21.62% 32 1.0821.081 −0.00075 99.93% 5.000 21.62% 41 1.082 1.081 −0.00059 99.95% 4.09526.41% 42 1.082 1.081 −0.00067 99.94% 4.095 26.40% 51 1.082 1.082−0.00021 99.98% 1.539 70.28% 52 1.082 1.081 −0.00069 99.94% 1.539 70.25%61 1.082 1.082 −0.00021 99.98% 5.000 21.63% 62 1.082 1.082 0.00005100.00% 5.000 21.64% 71 1.082 1.082 −0.00003 100.00% 4.933 21.93% 721.082 1.083 0.00083 100.08% 4.933 21.95% ARS ARS − (ARS/EHD) ARS/TP ARSEHD value EHD % TP (%) 11 20.767 21.486 0.719 103.46% 4.977 431.68% 129.412 13.474 4.062 143.16% 4.977 270.71% 21 8.636 9.212 0.577 106.68%5.000 184.25% 22 9.838 10.264 0.426 104.33% 5.000 205.27% 31 8.770 8.7720.003 100.03% 5.000 175.45% 32 8.511 8.558 0.047 100.55% 5.000 171.16%41 4.600 4.619 0.019 100.42% 4.095 112.80% 42 4.965 4.981 0.016 100.32%4.095 121.64% 51 5.075 5.143 0.067 101.33% 1.539 334.15% 52 5.047 5.0620.015 100.30% 1.539 328.89% 61 5.011 5.075 0.064 101.28% 5.000 101.50%62 5.373 5.489 0.116 102.16% 5.000 109.79% 71 5.513 5.625 0.112 102.04%4.933 114.03% 72 5.981 6.307 0.326 105.44% 4.933 127.84%

The results of the equations of the second optical embodiment based onTable 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second optical embodiment(Reference wavelength: 555 nm) HIF111 0 HIF111/HOI 0 SGI111 0 |SGI111|/0 (|SGI111| + TP1)

Third Optical Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing module ofthe third optical embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 310, asecond lens 320, a third lens 330, an aperture 300, a fourth lens 340, afifth lens 350, a sixth lens 360, a seventh lens 370, an IR-cut filter380, an image plane 390, and an image sensor 392.

The first lens 310 has negative refractive power and is made of glass.An object-side surface 312 thereof, which faces the object side, is aconvex spherical surface, and an image-side surface 314 thereof, whichfaces the image side, is a concave spherical surface.

The second lens 320 has negative refractive power and is made of glass.An object-side surface 322 thereof, which faces the object side, is aconcave spherical surface, and an image-side surface 324 thereof, whichfaces the image side, is a convex spherical surface.

The third lens 330 has positive refractive power and is made of plastic.An object-side surface 332 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 334 thereof, whichfaces the image side, is a convex aspheric surface. The image-sidesurface 334 has an inflection point.

The fourth lens 340 has negative refractive power and is made ofplastic. An object-side surface 342, which faces the object side, is aconcave aspheric surface, and an image-side surface 344, which faces theimage side, is a concave aspheric surface. The image-side surface 344has an inflection point.

The fifth lens 350 has positive refractive power and is made of plastic.An object-side surface 352, which faces the object side, is a convexaspheric surface, and an image-side surface 354, which faces the imageside, is a convex aspheric surface.

The sixth lens 360 has negative refractive power and is made of plastic.An object-side surface 362, which faces the object side, is a convexaspheric surface, and an image-side surface 364, which faces the imageside, is a concave aspheric surface. The object-side surface 362 has aninflection point, and the image-side surface 364 has an inflectionpoint. It may help to shorten the back focal length to keep small insize. Whereby, the incident angle of each view field entering the sixthlens 360 could be effectively adjusted to improve aberration.

The IR-cut filter 380 is made of glass and is disposed between the sixthlens 360 and the image plane 390. The IR-cut filter 390 gives nocontribution to the focal length of the optical image capturing module.

The parameters of the lenses of the third optical embodiment are listedin Table 5 and Table 6.

TABLE 5 f = 2.808 mm; f/HEP = 1.6; HAF = 100 deg Radius of curvatureThickness Refractive Abbe Focal length Surface (mm) (mm) Material indexnumber (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 71.398124 7.214 glass1.702 41.15 −11.765 2 7.117272355 5.788 3 2^(nd) lens −13.2921369910.000 glass 2.003 19.32 −4537.460 4 −18.37509887 7.005 5 3^(rd) lens5.039114804 1.398 plastic 1.514 56.80 7.553 6 −15.53136631 −0.140 7Aperture 1E+18 2.378 8 4^(th) lens −18.68613609 0.577 plastic 1.66120.40 −4.978 9 4.086545927 0.141 10 5^(th) lens 4.927609282 2.974plastic 1.565 58.00 4.709 11 −4.551946605 1.389 12 6^(th) lens9.184876531 1.916 plastic 1.514 56.80 −23.405 13 4.845500046 0.800 14Infrared 1E+18 0.500 BK_7 1.517 64.13 rays filter 15 1E+18 0.371 16Image 1E+18 0.005 plane Reference wavelength (d-line): 555 nm; theposition of blocking light: none.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 1.318519E−013.120384E+00 −1.494442E+01 A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 6.405246E−05 2.103942E−03 −1.598286E−03 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 2.278341E−05 −1.050629E−04−9.177115E−04 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−3.672908E−06 6.168906E−06 1.011405E−04 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 3.748457E−07 −1.224682E−07 −4.919835E−06Surface 9 10 11 12 13 k 2.744228E−02 −7.864013E+00 −2.263702E+00−4.206923E+01 −7.030803E+00 A4 −7.291825E−03 1.405243E−04 −3.919567E−03−1.679499E−03 −2.640099E−03 A6 9.730714E−05 1.837602E−04 2.683449E−04−3.518520E−04 −4.507651E−05 A8 1.101816E−06 −2.173368E−05 −1.229452E−055.047353E−05 −2.600391E−05 A10 −6.849076E−07 7.328496E−07 4.222621E−07−3.851055E−06 1.161811E−06

An equation of the aspheric surfaces of the third optical embodiment isthe same as that of the first optical embodiment, and the definitionsare the same as well.

The exact parameters of the third optical embodiment based on Table 5and Table 6 are listed in the following table:

Third optical embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.23865 0.00062 0.37172 0.56396 0.596210.11996 Σ PPR/|Σ TP4/ Σ PPR Σ NPR NPR| IN12/f IN56/f (IN34 + TP4 + IN45)1.77054 0.12058 14.68400 2.06169 0.49464 0.19512 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.00259 600.74778 1.30023 1.11131 HOS InTLHOS/HOI InS/HOS ODT % TDT % 42.31580 40.63970 10.57895 0.26115−122.32700 93.33510 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0 02.22299 2.60561 0.65140 0.06158 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 7.15374 2.42321 −0.20807 −0.24978 0.108610.13038 PhiA PhiC PhiD TH1 TH2 HOI 6.150 mm 6.41 mm 6.71 mm 0.15 mm 0.13mm 4 mm (TH1 + TH2)/ 2(TH1 + TH2)/ PhiA/PhiD TH1 + TH2 HOI (TH1 +TH2)/HOS PhiA InTL/HOS 0.9165 0.28 mm 0.07 0.0066 0.0911 0.9604 PSTAPLTA NSTA NLTA SSTA SLTA 0.014 mm 0.002 mm −0.003 mm −0.002 mm 0.011 mm−0.001 mm

The figures related to the profile curve lengths obtained based on Table5 and Table 6 are listed in the following table:

Third optical embodiment (Reference wavelength: 555 nm) ARE − 2(ARE/HEP)ARE 1/2(HEP) ARE value 1/2(HEP) % TP ARE/TP (%) 11 0.877 0.877 −0.00036 99.96% 7.214 12.16% 12 0.877 0.879 0.00186 100.21% 7.214 12.19% 210.877 0.878 0.00026 100.03% 10.000 8.78% 22 0.877 0.877 −0.00004 100.00%10.000 8.77% 31 0.877 0.882 0.00413 100.47% 1.398 63.06% 32 0.877 0.8770.00004 100.00% 1.398 62.77% 41 0.877 0.877 −0.00001 100.00% 0.577152.09% 42 0.877 0.883 0.00579 100.66% 0.577 153.10% 51 0.877 0.8810.00373 100.43% 2.974 29.63% 52 0.877 0.883 0.00521 100.59% 2.974 29.68%61 0.877 0.878 0.00064 100.07% 1.916 45.83% 62 0.877 0.881 0.00368100.42% 1.916 45.99% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP(%) 11 17.443  17.620  0.178 101.02% 7.214 244.25% 12 6.428 8.019 1.592124.76% 7.214 111.16% 21 6.318 6.584 0.266 104.20% 10.000 65.84% 226.340 6.472 0.132 102.08% 10.000 64.72% 31 2.699 2.857 0.158 105.84%1.398 204.38% 32 2.476 2.481 0.005 100.18% 1.398 177.46% 41 2.601 2.6520.051 101.96% 0.577 459.78% 42 3.006 3.119 0.113 103.75% 0.577 540.61%51 3.075 3.171 0.096 103.13% 2.974 106.65% 52 3.317 3.624 0.307 109.24%2.974 121.88% 61 3.331 3.427 0.095 102.86% 1.916 178.88% 62 3.944 4.1600.215 105.46% 1.916 217.14%

The results of the equations of the third optical embodiment based onTable 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third optical embodiment(Reference wavelength: 555 nm) HIF321 2.0367 HIF321/HOI 0.5092 SGI321−0.1056 |SGI321|/(|SGI321| + TP3) 0.0702 HIF421 2.4635 HIF421/HOI 0.6159SGI421 0.5780 |SGI421|/(|SGI421| + TP4) 0.5005 HIF611 1.2364 HIF611/HOI0.3091 SGI611 0.0668 |SGI611|/(|SGI611| + TP6) 0.0337 HIF621 1.5488HIF621/HOI 0.3872 SGI621 0.2014 |SGI621|/(|SGI621| + TP6) 0.0951

Fourth Optical Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing module 40 ofthe fourth optical embodiment of the present invention includes, alongan optical axis from an object side to an image side, a first lens 410,a second lens 420, an aperture 400, a third lens 430, a fourth lens 440,a fifth lens 450, an IR-cut filter 480, an image plane 490, and an imagesensor 492.

The first lens 410 has negative refractive power and is made of glass.An object-side surface 412 thereof, which faces the object side, is aconvex spherical surface, and an image-side surface 414 thereof, whichfaces the image side, is a concave spherical surface.

The second lens 420 has negative refractive power and is made ofplastic. An object-side surface 422 thereof, which faces the objectside, is a concave aspheric surface, and an image-side surface 424thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 422 has an inflection point.

The third lens 430 has positive refractive power and is made of plastic.An object-side surface 432 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 434 thereof, whichfaces the image side, is a convex aspheric surface. The object-sidesurface 432 has an inflection point.

The fourth lens 440 has positive refractive power and is made ofplastic. An object-side surface 442, which faces the object side, is aconvex aspheric surface, and an image-side surface 444, which faces theimage side, is a convex aspheric surface. The object-side surface 442has an inflection point.

The fifth lens 450 has negative refractive power and is made of plastic.An object-side surface 452, which faces the object side, is a concaveaspheric surface, and an image-side surface 454, which faces the imageside, is a concave aspheric surface. The object-side surface 452 has twoinflection points. It may help to shorten the back focal length to keepsmall in size.

The IR-cut filter 480 is made of glass and is disposed between the fifthlens 450 and the image plane 490. The IR-cut filter 480 gives nocontribution to the focal length of the optical image capturing module.

The parameters of the lenses of the fourth optical embodiment are listedin Table 7 and Table 8.

TABLE 7 f = 2.7883 mm; f/HEP = 1.8; HAF = 101 deg Radius of ThicknessRefractive Abbe Focal length Surface curvature (mm) (mm) Material indexnumber (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 76.84219 6.117399 glass1.497 81.61 −31.322 2 12.62555 5.924382 3 2^(nd) lens −37.0327 3.429817plastic 1.565 54.5 −8.70843 4 5.88556 5.305191 5 3^(rd) lens 17.9939514.79391 6 −5.76903 −0.4855 plastic 1.565 58 9.94787 7 Aperture 1E+180.535498 8 4^(th) lens 8.19404 4.011739 plastic 1.565 58 5.24898 9−3.84363 0.050366 10 5^(th) lens −4.34991 2.088275 plastic 1.661 20.4−4.97515 11 16.6609 0.6 12 Infrared 1E+18 0.5 BK_7 1.517 64.13 raysfilter 13 1E+18 3.254927 14 Image 1E+18 −0.00013 plane Referencewavelength (d-line): 555 nm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.131249 −0.069541 −0.324555 0.009216−0.292346 A4 0.000000E+00 0.000000E+00 3.99823E−05 −8.55712E−04−9.07093E−04 8.80963E−04 −1.02138E−03 A6 0.000000E+00 0.000000E+009.03636E−08 −1.96175E−06 −1.02465E−05 3.14497E−05 −1.18559E−04 A80.000000E+00 0.000000E+00 1.91025E−09 −1.39344E−08 −8.18157E−08−3.15863E−06     1.34404E−05 A10 0.000000E+00 0.000000E+00−1.18567E−11   −4.17090E−09 −2.42621E−09 1.44613E−07 −2.80681E−06 A120.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00  0.000000E+00 Surface 9 10 11 k −0.18604 −6.17195 27.541383A4 4.33629E−03   1.58379E−03   7.56932E−03 A6 −2.91588E−04  −1.81549E−04 −7.83858E−04 A8 9.11419E−06 −1.18213E−05   4.79120E−05 A101.28365E−07   1.92716E−06 −1.73591E−06 A12 0.000000E+00  0.000000E+000.000000E+00

An equation of the aspheric surfaces of the fourth optical embodiment isthe same as that of the first optical embodiment, and the definitionsare the same as well.

The exact parameters of the fourth optical embodiment based on Table 7and Table 8 are listed in the following table:

Fourth optical embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f1/f2| 0.08902 0.32019 0.28029 0.53121 0.560453.59674 Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN45/f |f2/f3| 1.4118 0.36933.8229 2.1247 0.0181 0.8754 TP3/(IN23 + TP3 + IN34) (TP1 + IN12)/TP2(TP5 + IN45)/TP4 0.73422 3.51091 0.53309 HOS InTL HOS/HOI InS/HOS ODT %TDT % 46.12590 41.77110 11.53148 0.23936 −125.266 99.1671 HVT52/ HVT41HVT42 HVT51 HVT52 HVT52/HOI HOS 0.00000 0.00000 0.00000 0.00000 0.000000.00000 TP2/TP3 TP3/TP4 InRS51 InRS52 |InRS51|/TP5 |InRS52|/TP5 0.231843.68765 −0.679265 0.5369 0.32528 0.25710 PhiA PhiC PhiD TH1 TH2 HOI5.598 mm 5.858 mm 6.118 mm 0.13 mm 0.13 mm 4 mm (TH1 + TH2)/ 2(TH1 +TH2)/ PhiA/PhiD TH1 + TH2 HOI (TH1 + TH2)/HOS PhiA InTL/HOS 0.9150 0.26mm 0.065 0.0056 0.0929 0.9056 PSTA PLTA NSTA NLTA SSTA SLTA −0.011 mm0.005 mm −0.010 mm −0.003 mm 0.005 mm −0.00026 mm

The figures related to the profile curve lengths obtained based on Table7 and Table 8 are listed in the following table:

Fourth optical embodiment (Reference wavelength: 555 nm) ARE ARE −2(ARE/ ARE/TP ARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 0.775 0.774−0.00052 99.93% 6.117 12.65% 12 0.775 0.774 −0.00005 99.99% 6.117 12.66%21 0.775 0.774 −0.00048 99.94% 3.430 22.57% 22 0.775 0.776 0.00168100.22% 3.430 22.63% 31 0.775 0.774 −0.00031 99.96% 14.794 5.23% 320.775 0.776 0.00177 100.23% 14.794 5.25% 41 0.775 0.775 0.00059 100.08%4.012 19.32% 42 0.775 0.779 0.00453 100.59% 4.012 19.42% 51 0.775 0.7780.00311 100.40% 2.088 37.24% 52 0.775 0.774 −0.00014 99.98% 2.088 37.08%ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD) % TP (%) 11 23.038 23.3970.359 101.56% 6.117 382.46% 12 10.140 11.772 1.632 116.10% 6.117 192.44%21 10.138 10.178 0.039 100.39% 3.430 296.74% 22 5.537 6.337 0.800114.44% 3.430 184.76% 31 4.490 4.502 0.012 100.27% 14.794 30.43% 322.544 2.620 0.076 102.97% 14.794 17.71% 41 2.735 2.759 0.024 100.89%4.012 68.77% 42 3.123 3.449 0.326 110.43% 4.012 85.97% 51 2.934 3.0230.089 103.04% 2.088 144.74% 52 2.799 2.883 0.084 103.00% 2.088 138.08%

The results of the equations of the fourth optical embodiment based onTable 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth optical embodiment(Reference wavelength: 555 nm) HIF211 6.3902 HIF211/HOI 1.5976 SGI211−0.4793 |SGI211|/(|SGI211| + TP2) 0.1226 HIF311 2.1324 HIF311/HOI 0.5331SGI311 0.1069 |SGI311|/(|SGI311| + TP3) 0.0072 HIF411 2.0278 HIF411/HOI0.5070 SGI411 0.2287 |SGI411|/(|SGI411| + TP4) 0.0539 HIF511 2.6253HIF511/HOI 0.6563 SGI511 −0.5681 |SGI511|/(|SGI511| + TP5) 0.2139 HIF5122.1521 HIF512/HOI 0.5380 SGI512 −0.8314 |SGI512|/(|SGI512| + TP5) 0.2848

Fifth Optical Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing module ofthe fifth optical embodiment of the present invention includes, along anoptical axis from an object side to an image side, an aperture 500, afirst lens 510, a second lens 520, a third lens 530, a fourth lens 540,an IR-cut filter 570, an image plane 580, and an image sensor 590.

The first lens 510 has positive refractive power and is made of plastic.An object-side surface 512, which faces the object side, is a convexaspheric surface, and an image-side surface 514, which faces the imageside, is a convex aspheric surface. The object-side surface 512 has aninflection point.

The second lens 520 has negative refractive power and is made ofplastic. An object-side surface 522 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 524thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 522 has two inflection points, and the image-sidesurface 524 has an inflection point.

The third lens 530 has positive refractive power and is made of plastic.An object-side surface 532, which faces the object side, is a concaveaspheric surface, and an image-side surface 534, which faces the imageside, is a convex aspheric surface. The object-side surface 532 hasthree inflection points, and the image-side surface 534 has aninflection point.

The fourth lens 540 has negative refractive power and is made ofplastic. An object-side surface 542, which faces the object side, is aconcave aspheric surface, and an image-side surface 544, which faces theimage side, is a concave aspheric surface. The object-side surface 542has two inflection points, and the image-side surface 544 has aninflection point.

The IR-cut filter 570 is made of glass and is disposed between thefourth lens 540 and the image plane 580. The IR-cut filter 570 gives nocontribution to the focal length of the optical image capturing module.

The parameters of the lenses of the fifth optical embodiment are listedin Table 9 and Table 10.

TABLE 9 f = 1.04102 mm; f/HEP = 1.4; HAF = 44.0346 deg Radius ofThickness Refractive Abbe Focal length Surface curvature (mm) (mm)Material index number (mm) 0 Object 1E+18 600 1 Aperture 1E+18 −0.020 21^(st) lens 0.890166851 0.210 plastic 1.545 55.96 1.587 3 −29.11040115−0.010 4 1E+18 0.116 5 2^(nd) lens 10.67765398 0.170 plastic 1.642 22.46−14.569 6 4.977771922 0.049 7 3^(rd) lens −1.191436932 0.349 plastic1.545 55.96 0.510 8 −0.248990674 0.030 9 4^(th) lens −38.08537212 0.176plastic 1.642 22.46 −0.569 10 0.372574476 0.152 11 1E+18 0.210 BK_71.517 64.13 1E+18 12 1E+18 0.185 1E+18 13 1E+18 0.005 1E+18 Referencewavelength (d-line): 555 nm; the position of blocking light: heeffective half diameter of the clear aperture of the fourth surface is0.360 mm.

TABLE 10 Coefficients of the aspheric surfaces Surface 2 3 5 6 7 8 k−1.106629E+00 2.994179E−07 −7.788754E+01 −3.440335E+01 −8.522097E−01−4.735945E+00 A4 8.291155E−01 −6.401113E−01 −4.958114E+00 −1.875957E+00−4.878227E−01 −2.490377E+00 A6 −2.398799E+01 −1.265726E+01 1.299769E+028.568480E+01 1.291242E+02 1.524149E+02 A8 1.825378E+02 8.457286E+01−2.736977E+03 −1.279044E+03 −1.979689E+03 −4.841033E+03 A10−6.211133E+02 −2.157875E+02 2.908537E+04 8.661312E+03 1.456076E+048.053747E+04 A12 −4.719066E+02 −6.203600E+02 −1.499597E+05 −2.875274E+04−5.975920E+04 −7.936887E+05 A14 0.000000E+00 0.000000E+00 2.992026E+053.764871E+04 1.351676E+05 4.811528E+06 A16 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 −1.329001E+05 −1.762293E+07 A18 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 3.579891E+07 A200.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−3.094006E+07 Surface 9 10 k −2.277155E+01 −8.039778E−01 A4 1.672704E+01−7.613206E+00 A6 −3.260722E+02 3.374046E+01 A8 3.373231E+03−1.368453E+02 A10 −2.177676E+04 4.049486E+02 A12 8.951687E+04−9.711797E+02 A14 −2.363737E+05 1.942574E+03 A16 3.983151E+05−2.876356E+03 A18 −4.090689E+05 2.562386E+03 A20 2.056724E+05−9.943657E+02

An equation of the aspheric surfaces of the fifth optical embodiment isthe same as that of the first optical embodiment, and the definitionsare the same as well.

The exact parameters of the fifth optical embodiment based on Table 9and

Fifth optical embodiment (Reference wavelength: 555 nm) InRS41 InRS42HVT41 HVT42 ODT % TDT % −0.07431 0.00475 0.00000 0.53450 2.09403 0.84704|f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3| 0.65616 0.07145 2.041291.83056 0.10890 28.56826 Σ PPR Σ NPR Σ PPR/|Σ NPR| Σ PP Σ NP f1/Σ PP2.11274 2.48672 0.84961 −14.05932 1.01785 1.03627 f4/Σ NP IN12/f IN23/fIN34/f TP3/f TP4/f 1.55872 0.10215 0.04697 0.02882 0.33567 0.16952 InTLHOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.09131 1.64329 1.59853 0.987830.66410 0.83025 (TP1 + IN12)/ (TP4 + IN34)/ TP2 TP3 TP1/TP2 TP3/TP4IN23/(TP2 + IN23 + TP3) 1.86168 0.59088 1.23615 1.98009 0.08604|InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS InTL/HOS 0.4211 0.02690.5199 0.3253 0.6641 PhiA PhiC PhiD TH1 TH2 HOI 1.596 mm 1.996 mm 2.396mm 0.2 mm 0.2 mm 1.028 mm (TH1 + TH2)/ (TH1 + TH2)/ 2(TH1 + TH2)/PhiA/PhiD TH1 + TH2 HOI HOS PhiA 0.7996 0.4 mm 0.3891 0.2434 0.5013 PSTAPLTA NSTA NLTA SSTA SLTA −0.029 mm −0.023 mm −0.011 mm −0.024 mm 0.010mm 0.011 mm

The results of the equations of the fifth optical embodiment based onTable 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth optical embodiment(Reference wavelength: 555 nm) HIF111 0.28454 HIF111/HOI 0.27679 SGI1110.04361 |SGI111|/(|SGI111| + TP1) 0.17184 HIF211 0.04198 HIF211/HOI0.04083 SGI211 0.00007 |SGI211|/(|SGI211| + TP2) 0.00040 HIF212 0.37903HIF212/HOI 0.36871 SGI212 −0.03682 |SGI212|/(|SGI212| + TP2) 0.17801HIF221 0.25058 HIF221/HOI 0.24376 SGI221 0.00695 |SGI221|/(|SGI221| +TP2) 0.03927 HIF311 0.14881 HIF311/HOI 0.14476 SGI311 −0.00854|SGI311|/(|SGI311| + TP3) 0.02386 HIF312 0.31992 HIF312/HOI 0.31120SGI312 −0.01783 |SGI312|/(|SGI312| + TP3) 0.04855 HIF313 0.32956HIF313/HOI 0.32058 SGI313 −0.01801 |SGI313|/(|SGI313| + TP3) 0.04902HIF321 0.36943 HIF321/HOI 0.35937 SGI321 −0.14878 |SGI321|/(|SGI321| +TP3) 0.29862 HIF411 0.01147 HIF411/HOI 0.01116 SGI411 −0.00000|SGI411|/(|SGI411| + TP4) 0.00001 HIF412 0.22405 HIF412/HOI 0.21795SGI412 0.01598 |SGI412|/(|SGI412| + TP4) 0.08304 HIF421 0.24105HIF421/HOI 0.23448 SGI421 0.05924 |SGI421|/(|SGI421| + TP4) 0.25131

The figures related to the profile curve lengths obtained based on Table9 and Table 10 are listed in the following table:

Fifth optical embodiment (Reference wavelength: 555 nm) ARE − ARE1/2(HEP) ARE value 1/2(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 0.368 0.3740.00578 101.57% 0.210 178.10% 12 0.366 0.368 0.00240 100.66% 0.210175.11% 21 0.372 0.375 0.00267 100.72% 0.170 220.31% 22 0.372 0.371−0.00060    99.84% 0.170 218.39% 31 0.372 0.372 −0.00023    99.94% 0.349106.35% 32 0.372 0.404 0.03219 108.66% 0.349 115.63% 41 0.372 0.3730.00112 100.30% 0.176 211.35% 42 0.372 0.387 0.01533 104.12% 0.176219.40% ARS − ARS EHD ARS value EHD (ARS/EHD) % TP ARS/TP (%) 11 0.3680.374 0.00578 101.57% 0.210 178.10% 12 0.366 0.368 0.00240 100.66% 0.210175.11% 21 0.387 0.391 0.00383 100.99% 0.170 229.73% 22 0.458 0.4600.00202 100.44% 0.170 270.73% 31 0.476 0.478 0.00161 100.34% 0.349136.76% 32 0.494 0.538 0.04435 108.98% 0.349 154.02% 41 0.585 0.6240.03890 106.65% 0.176 353.34% 42 0.798 0.866 0.06775 108.49% 0.176490.68%

Sixth Optical Embodiment

As shown in FIG. 7A and FIG. 7B, an optical image capturing module ofthe sixth optical embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 610, anaperture 600, a second lens 620, a third lens 630, an IR-cut filter 670,an image plane 680, and an image sensor 690.

The first lens 610 has positive refractive power and is made of plastic.An object-side surface 612, which faces the object side, is a convexaspheric surface, and an image-side surface 614, which faces the imageside, is a concave aspheric surface.

The second lens 620 has negative refractive power and is made ofplastic. An object-side surface 622 thereof, which faces the objectside, is a concave aspheric surface, and an image-side surface 624thereof, which faces the image side, is a convex aspheric surface. Theimage-side surface 624 has an inflection point.

The third lens 630 has positive refractive power and is made of plastic.An object-side surface 632, which faces the object side, is a convexaspheric surface, and an image-side surface 634, which faces the imageside, is a concave aspheric surface. The object-side surface 632 has twoinflection points, and the image-side surface 634 has an inflectionpoint.

The IR-cut filter 670 is made of glass and is disposed between the thirdlens 630 and the image plane 680. The IR-cut filter 670 gives nocontribution to the focal length of the optical image capturing module.

The parameters of the lenses of the sixth optical embodiment are listedin Table 11 and Table 12.

TABLE 11 f = 2.41135 mm; f/HEP = 2.22; HAF = 36 deg Radius of ThicknessRefractive Abbe Focal length Surface curvature (mm) (mm) Material indexnumber (mm) 0 Object 1E+18 600 1 1^(st) lens 0.840352226 0.468 plastic1.535 56.27 2.232 2 2.271975602 0.148 3 Aperture 1E+18 0.277 4 2^(nd)lens −1.157324239 0.349 plastic 1.642 22.46 −5.221 5 −1.968404008 0.2216 3^(rd) lens 1.151874235 0.559 plastic 1.544 56.09 7.360 7 1.3381051590.123 8 Infrared 1E+18 0.210 BK7 1.517 64.13 rays filter 9 1E+18 0.54710 Image 1E+18 0.000 plane Reference wavelength (d-line): 555 nm; theposition of blocking light: the effective half diameter of the clearaperture of the first surface is 0.640 mm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 k−2.019203E−01 1.528275E+01 3.743939E+00 −1.207814E+01 −1.276860E+01−3.034004E+00 A4 3.944883E−02 −1.670490E−01 −4.266331E−01 −1.696843E+00−7.396546E−01 −5.308488E−01 A6 4.774062E−01 3.857435E+00 −1.423859E+005.164775E+00 4.449101E−01 4.374142E−01 A8 −1.528780E+00 −7.091408E+014.119587E+01 −1.445541E+01 2.622372E−01 −3.111192E−01 A10 5.133947E+006.365801E+02 −3.456462E+02 2.876958E+01 −2.510946E−01 1.354257E−01 A12−6.250496E+00 −3.141002E+03 1.495452E+03 −2.662400E+01 −1.048030E−01−2.652902E−02 A14 1.068803E+00 7.962834E+03 −2.747802E+03 1.661634E+011.462137E−01 −1.203306E−03 A16 7.995491E+00 −8.268637E+03 1.443133E+03−1.327827E+01 −3.676651E−02 7.805611E−04

An equation of the aspheric surfaces of the sixth optical embodiment isthe same as that of the first optical embodiment, and the definitionsare the same as well.

The exact parameters of the sixth optical embodiment based on Table 11and Table 12 are listed in the following table:

Sixth optical embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f1/f2| |f2/f3| TP1/TP2 1.08042 0.46186 0.32763 2.33928 1.409681.33921 Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN23/f TP2/TP3 1.40805 0.461863.04866 0.17636 0.09155 0.62498 TP2/ (IN12 + TP2 + IN23) (TP1 +IN12)/TP2 (TP3 + IN23)/TP2 0.35102 2.23183 2.23183 HOS InTL HOS/HOIInS/HOS |ODT|% |TDT|% 2.90175 2.02243 1.61928 0.78770 1.50000 0.71008HVT32/ HVT21 HVT22 HVT31 HVT32 HVT32/HOI HOS 0.00000 0.00000 0.468870.67544 0.37692 0.23277 PhiA PhiC PhiD TH1 TH2 HOI 2.716 mm 3.116 mm3.616 mm 0.25 mm 0.2 mm 1.792 mm PhiA/ (TH1 + TH2)/ (TH1 + TH2)/ PhiDTH1 + TH2 HOI HOS 2(TH1 + TH2)/PhiA InTL/HOS 0.7511 0.45 mm 0.25110.1551 0.3314 0.6970 PLTA PSTA NLTA NSTA SLTA SSTA −0.002 mm 0.008 mm0.006 mm −0.008 mm −0.007 mm 0.006 mm

The results of the equations of the sixth optical embodiment based onTable 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth optical embodiment(Reference wavelength: 555 nm) HIF221 0.5599 HIF221/HOI 0.3125 SGI221−0.1487 |SGI221|/(|SGI221| + TP2) 0.2412 HIF311 0.2405 HIF311/HOI 0.1342SGI311 0.0201 |SGI311|/(|SGI311| + TP3) 0.0413 HIF312 0.8255 HIF312/HOI0.4607 SGI312 −0.0234 |SGI312|/(|SGI312| + TP3) 0.0476 HIF321 0.3505HIF321/HOI 0.1956 SGI321 0.0371 |SGI321|/(|SGI321| + TP3) 0.0735

The figures related to the profile curve lengths obtained based on Table11 and Table 12 are listed in the following table:

Sixth optical embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ARE 1/2(HEP) value 1/2(HEP) HEP) % TP ARE/TP (%) 11 0.546 0.598 0.052109.49% 0.468 127.80% 12 0.500 0.506 0.005 101.06% 0.468 108.03% 210.492 0.528 0.036 107.37% 0.349 151.10% 22 0.546 0.572 0.026 104.78%0.349 163.78% 31 0.546 0.548 0.002 100.36% 0.559  98.04% 32 0.546 0.5500.004 100.80% 0.559  98.47% ARS (ARS/ ARS EHD value ARS − EHD EHD) % TPARS/TP (%) 11 0.640 0.739 0.099 115.54% 0.468 158.03% 12 0.500 0.5060.005 101.06% 0.468 108.03% 21 0.492 0.528 0.036 107.37% 0.349 151.10%22 0.706 0.750 0.044 106.28% 0.349 214.72% 31 1.118 1.135 0.017 101.49%0.559 203.04% 32 1.358 1.489 0.131 109.69% 0.559 266.34%

The optical image capturing module of the present invention could be oneof a group consisting of an electronic portable device, an electronicwearable device, an electronic monitoring device, an electronicinformation device, an electronic communication device, a machine visiondevice, and a vehicle electronic device. In addition, the optical imagecapturing module of the present invention could reduce the requiredmechanism space and increase the visible area of the screen by usingdifferent lens groups with different number of lens.

As shown in FIG. 8A, an optical image capturing module 712 and anoptical image capturing module 714 (front lens) of the present inventionare applied to a mobile communication device 71 (e.g. a smart phone). Asshown in FIG. 8B, an optical image capturing module 722 of the presentinvention is applied to a mobile information device 72 (e.g. anotebook). As shown in FIG. 8C, an optical image capturing module 732 ofthe present invention is applied to a smart watch 73. As shown in FIG.8D, an optical image capturing module 742 of the present invention isapplied to a smart head-wearing device 74 (e.g. a smart hat). As shownin FIG. 8E, an optical image capturing module 752 of the presentinvention is applied to a safety monitoring device 75 (e.g. an IP cam).As shown in FIG. 8F, an optical image capturing module 762 of thepresent invention is applied to a vehicle image device 76. As shown inFIG. 8G, an optical image capturing module 772 of the present inventionis applied to an unmanned aircraft device 77. As shown in FIG. 8H, anoptical image capturing module 782 of the present invention is appliedto an extreme sport image device 78.

It must be pointed out that the embodiments described above are onlysome embodiments of the present invention. All equivalent structureswhich employ the concepts disclosed in this specification and theappended claims should fall within the scope of the present invention.

What is claimed is:
 1. An optical image capturing module, comprising: acircuit assembly, which comprises a circuit substrate, a sensor holder,and an image sensing component, wherein the circuit substrate has aplurality of circuit contacts thereon; the image sensing component has afirst surface and a second surface, wherein the first surface isconnected to the circuit substrate; the second surface has a sensingsurface and a plurality of image contacts; each of the image contacts iselectrically connected to one of the circuit contacts on the circuitsubstrate via a plurality of signal transmission elements; the sensorholder is disposed on the circuit substrate and on the second surface ofthe image sensing component, and covers the circuit contacts and theimage contacts; the signal transmission elements are embedded in thesensor holder; and a lens assembly, which comprises a lens base and alens group, wherein the lens base is made of an opaque material and hasa receiving hole penetrating through two ends of the lens base, so thatthe lens base is hollow; in addition, the lens base is disposed on thesensor holder, so that the receiving hole directly faces the imagesensing component; the lens group comprises at least two lenses havingrefractive power, and is disposed on the lens base and is located in thereceiving hole; moreover, an image plane of the lens group is located onthe sensing surface, and an optical axis of the lens group overlaps witha central normal of the sensing surface, so that a light passes throughthe lens group in the receiving hole and projects onto the sensingsurface; wherein the optical image capturing module satisfies:1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; 0 mm<PhiD≤18 mm; 0<PhiA/PhiD≤0.99;and 0.9≤2(ARE/HEP)≤2.0; where f is a focal length of the lens group; HEPis an entrance pupil diameter of the lens group; HAF is a half of amaximum field angle of the lens group; PhiD is a maximum value of aminimum length on a periphery of the lens base perpendicular to theoptical axis of the lens group; PhiA is a maximum effective diameter ofan image-side surface of the at least two lenses of the lens groupclosest to the image plane; ARE is a profile curve length measured froma start point where the optical axis of the lens group passes throughany surface of one of the at least two lenses, along a surface profileof the corresponding lens, and finally to a coordinate point of aperpendicular distance where is a half of the entrance pupil diameteraway from the optical axis.
 2. The optical image capturing module ofclaim 1, wherein the optical image capturing module further satisfies:0.9≤ARS/EHD≤2.0; where for any surface of any lens, ARS is a profilecurve length measured from a start point where the optical axis passestherethrough, along a surface profile thereof, and finally to an endpoint of the maximum effective half diameter thereof; EHD is a maximumeffective half diameter thereof.
 3. The optical image capturing moduleof claim 1, wherein the optical image capturing module furthersatisfies: PLTA≤100 μm; PSTA≤100 μm; NLTA≤100 μm; NSTA≤100 μm; SLTA≤100μm; SSTA≤100 μm; and |TDT|<250% where HOI is a maximum height for imageformation perpendicular to the optical axis on the image plane; PLTA isa transverse aberration at 0.7 HOI in a positive direction of atangential ray fan aberration after the longest operation wavelengthpassing through an edge of the entrance pupil; PSTA is a transverseaberration at 0.7 HOI in the positive direction of the tangential rayfan aberration after the shortest operation wavelength passing throughthe edge of the entrance pupil; NLTA is a transverse aberration at 0.7HOI in a negative direction of the tangential ray fan aberration afterthe longest operation wavelength passing through the edge of theentrance pupil; NSTA is a transverse aberration at 0.7 HOI in thenegative direction of the tangential ray fan aberration after theshortest operation wavelength passing through the edge of the entrancepupil; SLTA is a transverse aberration at 0.7 HOI of a sagittal ray fanaberration after the longest operation wavelength passing through theedge of the entrance pupil; SSTA is a transverse aberration at 0.7 HOIof the sagittal ray fan aberration after the shortest operationwavelength passing through the edge of the entrance pupil; TDT is a TVdistortion for image formation in the optical image capturing module. 4.The optical image capturing module of claim 1, wherein the lens groupcomprises four lenses having refractive power, which are constituted bya first lens, a second lens, a third lens, and a fourth lens in orderalong an optical axis from an object side to an image side; the lensgroup satisfies: 0.1≤InTL/HOS≤0.95; where HOS is a distance in parallelwith the optical axis between an object-side surface of the first lensand the image plane; InTL is a distance in parallel with the opticalaxis from the object-side surface of the first lens to an image-sidesurface of the fourth lens.
 5. The optical image capturing module ofclaim 1, wherein the lens group comprises five lenses having refractivepower, which are constituted by a first lens, a second lens, a thirdlens, a fourth lens, and a fifth lens in order along an optical axisfrom an object side to an image side; the lens group satisfies:0.1≤InTL/HOS≤0.95; where HOS is a distance in parallel with the opticalaxis between an object-side surface of the first lens and the imageplane; InTL is a distance in parallel with the optical axis from theobject-side surface of the first lens to an image-side surface of thefifth lens.
 6. The optical image capturing module of claim 1, whereinthe lens group comprises six lenses having refractive power, which areconstituted by a first lens, a second lens, a third lens, a fourth lens,a fifth lens, and a six lens in order along an optical axis from anobject side to an image side; the lens group satisfies:0.1≤InTL/HOS≤0.95; where HOS is a distance in parallel with the opticalaxis between an object-side surface of the first lens and the imageplane; InTL is a distance in parallel with the optical axis from theobject-side surface of the first lens to an image-side surface of thesixth lens.
 7. The optical image capturing module of claim 1, whereinthe lens group comprises seven lenses having refractive power, which areconstituted by a first lens, a second lens, a third lens, a fourth lens,a fifth lens, a sixth lens, and a seventh lens in order along an opticalaxis from an object side to an image side; the lens group satisfies:0.1≤InTL/HOS≤0.95; where HOS is a distance in parallel with the opticalaxis between an object-side surface of the first lens and the imageplane; InTL is a distance in parallel with the optical axis from theobject-side surface of the first lens to an image-side surface of theseventh lens.
 8. The optical image capturing module of claim 1, whereinthe optical image capturing module further satisfies: MTFQ0≥0.2;MTFQ3≥0.01; and MTFQ7≥0.01; where HOI is a maximum height for imageformation perpendicular to the optical axis on the image plane; MTFQ0,MTFQ3, and MTFQ7 are respectively a value of modulation transferfunction of visible light in a spatial frequency of 110 cycles/mm at theoptical axis, 0.3 HOI, and 0.7 HOI on an image plane for visible light.9. The optical image capturing module of claim 1, further comprising anaperture, wherein the optical image capturing module further satisfies:0.2≤InS/HOS≤1.1; where InS is a distance on the optical axis between theaperture and the image plane; HOS is a distance in parallel with theoptical axis between an object-side surface of one of the at least twolenses of the lens group furthest from the image plane and the imageplane.
 10. The optical image capturing module of claim 1, wherein thelens base further comprises a lens barrel and a lens holder; the lensholder has a lower through hole penetrating through two ends of the lensholder, so that the image sensing component is located in the lowerthrough hole; the lens barrel is disposed in the lens holder and islocated in the lower through hole, and has an upper through holepenetrating through two ends of the lens barrel, so that the upperthrough hole communicates with the lower through hole to form thereceiving hole; the lens base is firmly disposed on the sensor holder;the upper through hole of the lens barrel directly faces the sensingsurface of the image sensing component; in addition, the lens group isdisposed in the lens barrel to be located in the upper through hole;PhiD is a maximum value of a minimum length on a periphery of the lensholder perpendicular to an optical axis of the lens group.
 11. Theoptical image capturing module of claim 10, wherein the optical imagecapturing module further satisfies: 0 mm<TH1+TH2≤1.5 mm; where TH1 is amaximum thickness of the lens holder; TH2 is a minimum thickness of thelens barrel.
 12. The optical image capturing module of claim 10, whereinthe optical image capturing module further satisfies:0<(TH1+TH2)/HOI≤0.95; where TH1 is a maximum thickness of the lensholder; TH2 is a minimum thickness of the lens barrel; HOI is a maximumheight for image formation perpendicular to the optical axis on theimage plane.
 13. The optical image capturing module of claim 10, whereinan outer peripheral wall of the lens barrel has an external threadthereon, and an inner wall of the lower through hole has an inner threadthereon, wherein the inner thread is screwed with the external thread,so that the lens barrel is disposed in the lens holder to be fixed inthe lower through hole.
 14. The optical image capturing module of claim10, wherein a glue is coated between the lens barrel and the lensholder, and the lens barrel and the lens holder are fixed to each othervia the glue, so that the lens barrel is disposed in the lens holder andis fixed in the lower through hole.
 15. The optical image capturingmodule of claim 1, wherein the lens base is integrally formed as amonolithic unit.
 16. The optical image capturing module of claim 15,wherein the optical image capturing module further comprises an IR-cutfilter which is disposed in the lens base or on the sensor holder to belocated above the image sensing component.
 17. The optical imagecapturing module of claim 10, wherein the optical image capturing modulefurther comprises an IR-cut filter which is disposed in the lens barrel,in the lens holder, or on the sensor holder to be located above theimage sensing component.
 18. The optical image capturing module of claim1, wherein the optical image capturing module further comprises anIR-cut filter; the lens base comprises a filter holder; the filterholder has a through hole penetrating through two ends of the filterholder; the IR-cut filter is disposed in the filter holder and islocated in the through hole of the filter holder; the filter holder isdisposed on the sensor holder, so that the IR-cut filter is locatedabove the image sensing component.
 19. The optical image capturingmodule of claim 18, wherein the lens base further comprises a lensbarrel and a lens holder; the lens barrel has an upper through holepenetrating through two ends of the lens barrel, and the lens holder hasa lower through hole penetrating through two ends of the lens holder;the lens barrel is disposed in the lens holder and is located in thelower through hole, and the lens holder is fixed on the filter holder,so that the upper through hole, the lower through hole, and the throughhole of the filter holder communicate with one another to form thereceiving hole; the upper through hole of the lens barrel directly facesthe sensing surface of the image sensing component; in addition, thelens group is disposed in the lens barrel to be located in the upperthrough hole; PhiD is a maximum value of a minimum length on a peripheryof the lens holder perpendicular to an optical axis of the lens group.20. The optical image capturing module of claim 19, wherein the opticalimage capturing module further satisfies: 0 mm<TH1+TH2≤1.5 mm; where TH1is a maximum thickness of the lens holder; TH2 is a minimum thickness ofthe lens barrel.
 21. The optical image capturing module of claim 19,wherein the optical image capturing module further satisfies:0<(TH1+TH2)/HOI≤0.95; where TH1 is a maximum thickness of the lensholder; TH2 is a minimum thickness of the lens barrel; HOI is a maximumheight for image formation perpendicular to the optical axis on theimage plane.
 22. The optical image capturing module of claim 19, whereinan outer peripheral wall of the lens barrel has an external threadthereon, and an inner wall of the lower through hole has an inner threadthereon, wherein the inner thread is screwed with the external thread,so that the lens barrel is disposed in the lens holder and is located inthe lower through hole; in addition, a glue is coated between the lensholder and the filter holder, and the lens holder and the filter holderare fixed to each other via the glue, so that the lens holder is fixedon the filter holder.
 23. The optical image capturing module of claim19, wherein a glue is coated between the lens barrel and the lensholder, and the lens barrel and the lens holder are fixed to each othervia the glue, so that the lens barrel is disposed in the lens holder andis located in the lower through hole; in addition, a glue is coatedbetween the lens holder and the filter holder, and the lens holder andthe filter holder are fixed to each other via the glue, so that the lensholder is fixed on the filter holder.
 24. The optical image capturingmodule of claim 1, wherein the optical image capturing module is appliedto one of a group consisting of an electronic portable device, anelectronic wearable device, an electronic monitoring device, anelectronic information device, an electronic communication device, amachine vision device, and a vehicle electronic device.